Ultrafast Sintering of Solid-State Electrolytes with Volatile Fillers
Source abstract
Abstract
Enhancing the performance of ceramic solid-state electrolytes (SSEs) often relies on incorporating effective fillers. However, the choice of fillers is often limited to only a few highly stable ones, as the long-term sintering by conventional methods often leads to severe loss of volatile components. Herein, we develop an ultrafast sintering method for SSEs with volatile fillers toward a dense and high-performance membrane. Using Ta-doped Li7La3Zr2O12 (LLZTO) as a model system, we sinter a Li3N/LLZTO composite SSE, which shows a higher relative density, a higher ionic conductivity, and a reduced electronic conductivity compared to the pristine LLZTO. In contrast, no Li3N can be observed in the membrane sintered by a conventional furnace due to its high volatility. This study opens up a new route for the rational selection of fillers in a much broader space toward synthesizing high-quality and high-performance ceramic SSEs.
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
Department of Materials Science and Engineering, University of Maryland, College Park, Maryland 20742, United States
Department of NanoEngineering, University of California San Diego, La Jolla, California 92093, United States
Center for Materials Innovation, University of Maryland, College Park, Maryland 20742, United States
References (43)
Show source-provided references
1. 10.1021/ja309143810.1021/ja3091438 ↗
2. 10.1038/s41560-019-0405-310.1038/s41560-019-0405-3 ↗
3. 10.1038/s41560-020-00759-510.1038/s41560-020-00759-5 ↗
4. 10.1038/s41578-020-00261-010.1038/s41578-020-00261-0 ↗
5. 10.1038/s41560-020-0597-610.1038/s41560-020-0597-6 ↗
6. 10.1016/j.jpowsour.2010.01.07610.1016/j.jpowsour.2010.01.076 ↗
7. 10.1002/adma.20190622110.1002/adma.201906221 ↗
8. 10.1126/science.aaz768110.1126/science.aaz7681 ↗
9. 10.1016/j.ceramint.2012.10.20610.1016/j.ceramint.2012.10.206 ↗
10. 10.1016/j.jpowsour.2018.04.02210.1016/j.jpowsour.2018.04.022 ↗
11. 10.1039/C8EE00540K10.1039/C8EE00540K ↗
12. 10.1021/acsenergylett.8b0024910.1021/acsenergylett.8b00249 ↗
13. 10.1038/s41563-021-01019-x10.1038/s41563-021-01019-x ↗
14. 10.1021/acsenergylett.9b0266010.1021/acsenergylett.9b02660 ↗
15. 10.1021/acsenergylett.0c0231410.1021/acsenergylett.0c02314 ↗
16. 10.1002/aenm.20190067110.1002/aenm.201900671 ↗
17. 10.1021/acsaem.9b0143110.1021/acsaem.9b01431 ↗
18. 10.1016/j.jpowsour.2014.04.06510.1016/j.jpowsour.2014.04.065 ↗
19. 10.1111/jace.1457210.1111/jace.14572 ↗
20. 10.1016/j.jechem.2019.02.00310.1016/j.jechem.2019.02.003 ↗
21. 10.1002/anie.20160892410.1002/anie.201608924 ↗
22. 10.1016/j.electacta.2018.08.07910.1016/j.electacta.2018.08.079 ↗
23. 10.1016/j.jpowsour.2017.04.02610.1016/j.jpowsour.2017.04.026 ↗
24. 10.1016/j.ceramint.2021.03.13810.1016/j.ceramint.2021.03.138 ↗
25. 10.1016/j.ceramint.2019.04.19210.1016/j.ceramint.2019.04.192 ↗
26. 10.1126/sciadv.abc864110.1126/sciadv.abc8641 ↗
27. 10.1021/acscentsci.7b0048010.1021/acscentsci.7b00480 ↗
28. 10.1038/s41560-019-0384-410.1038/s41560-019-0384-4 ↗
29. 10.1039/c0ee00052c10.1039/c0ee00052c ↗
30. 10.1016/j.mattod.2020.10.00210.1016/j.mattod.2020.10.002 ↗
31. 10.1007/s10853-008-3008-010.1007/s10853-008-3008-0 ↗
32. 10.1111/jace.1528810.1111/jace.15288 ↗
33. 10.1016/j.ssi.2013.09.00510.1016/j.ssi.2013.09.005 ↗
34. 10.1002/aenm.20170073210.1002/aenm.201700732 ↗
35. 10.1002/adfm.20200638110.1002/adfm.202006381 ↗
36. 10.1002/anie.20191441710.1002/anie.201914417 ↗
37. 10.1002/anie.20200054710.1002/anie.202000547 ↗
38. 10.1021/jacs.8b0310610.1021/jacs.8b03106 ↗
39. 10.1038/s41560-018-0312-z10.1038/s41560-018-0312-z ↗
40. 10.1039/C9TA10269H10.1039/C9TA10269H ↗
41. 10.1016/j.ssi.2015.01.00410.1016/j.ssi.2015.01.004 ↗
42. 10.1021/acsenergylett.9b0184710.1021/acsenergylett.9b01847 ↗
43. 10.1021/jacs.0c0488710.1021/jacs.0c04887 ↗