Giant Energy-Storage Density and Thermally Activated Phase Transition in (Pb0.96La0.04)(Zr0.99Ti0.01)O3 Antiferroelectric Ceramics
Source abstract
Abstract
Antiferroelectric materials are regarded as potential energy storage materials due to their superior energy density during the antiferroelectric to ferroelectric phase transition. Nevertheless, their unsatisfactory energy density limits their application in practice. Herein, (Pb0.96La0.04)(Zr0.99Ti0.01)O3 (PLZT) antiferroelectric ceramics are prepared via a tape-casting technique. Interestingly, the tape-casting technique can improve the ceramic microstructure, which leads to breakdown strengths ranging from 336 kV/cm for a solid state reaction to 400 kV/cm for tape-casting. A giant recoverable energy density of 11.38 J/cm3 is realized at 395 kV/cm. Meanwhile, for PLZT ceramics, a high discharge energy density of 6.2 J/cm3 and fast discharge speed (t0.9 = 69 ns) are achieved simultaneously under 350 kV/cm. Furthermore, the thermally activated antiferroelectric behavior is observed in P–E loops, and a high energy density of 8.3 J/cm3 is realized at 60 °C and 310 kV/cm. Therefore, these excellent properties demonstrate that PLZT antiferroelectric materials are a potential candidate in advanced power electronic devices.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Ferroelectric and Piezoelectric Materials · Multiferroics and related materials · Dielectric materials and actuators
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Inner Mongolia Key Laboratory of Ferroelectric-related New Energy Materials and Devices, Inner Mongolia University of Science and Technology, Baotou 014010, China
Key Laboratory of Integrated Exploitation of Bayan Obo Multi-Metal Resources, Inner Mongolia University of Science and Technology, Baotou 014010, China
Funding
Inner Mongolia Autonomous Region · Plan Project for Science and Technology of Baotou
References (36)
Show source-provided references
1. 10.1111/jace.1687810.1111/jace.16878 ↗
2. 10.1016/j.cej.2020.12487910.1016/j.cej.2020.124879 ↗
3. 10.1016/j.jeurceramsoc.2018.09.03910.1016/j.jeurceramsoc.2018.09.039 ↗
4. 10.1016/j.ensm.2020.05.02610.1016/j.ensm.2020.05.026 ↗
5. 10.1111/jace.1539210.1111/jace.15392 ↗
6. 10.1002/adma.20170182410.1002/adma.201701824 ↗
7. 10.1111/jace.1373710.1111/jace.13737 ↗
8. 10.1021/acs.chemmater.8b0447010.1021/acs.chemmater.8b04470 ↗
9. 10.1016/j.ceramint.2012.12.07110.1016/j.ceramint.2012.12.071 ↗
10. 10.1021/acsaem.8b0109910.1021/acsaem.8b01099 ↗
11. 10.1038/s41467-020-18665-510.1038/s41467-020-18665-5 ↗
12. 10.1016/j.nanoen.2020.10542310.1016/j.nanoen.2020.105423 ↗
13. 10.1039/C8TA12232F10.1039/C8TA12232F ↗
14. 10.1039/D0EE02104K10.1039/D0EE02104K ↗
15. 10.1021/acsaem.9b0155010.1021/acsaem.9b01550 ↗
16. 10.1111/jace.1440610.1111/jace.14406 ↗
17. 10.1002/aelm.20190136610.1002/aelm.201901366 ↗
18. 10.1016/j.jallcom.2014.09.17110.1016/j.jallcom.2014.09.171 ↗
19. 10.1111/jace.1766910.1111/jace.17669 ↗
20. 10.1039/C8TC03003K10.1039/C8TC03003K ↗
21. 10.1021/acsaem.9b0066410.1021/acsaem.9b00664 ↗
22. 10.1039/C9TA02149C10.1039/C9TA02149C ↗
23. 10.1039/C8EE03287D10.1039/C8EE03287D ↗
24. 10.1016/j.pmatsci.2018.12.00510.1016/j.pmatsci.2018.12.005 ↗
25. 10.1016/j.ceramint.2017.06.00510.1016/j.ceramint.2017.06.005 ↗
26. 10.1021/acsami.0c0987610.1021/acsami.0c09876 ↗
27. 10.1063/1.497342510.1063/1.4973425 ↗
28. 10.1021/acsaem.9b0155010.1021/acsaem.9b01550 ↗
29. 10.1016/j.nanoen.2020.10501210.1016/j.nanoen.2020.105012 ↗
30. 10.1021/acssuschemeng.7b0220310.1021/acssuschemeng.7b02203 ↗
31. 10.1002/adfm.20180732110.1002/adfm.201807321 ↗
32. 10.1111/jace.1491210.1111/jace.14912 ↗
33. 10.1007/s10854-019-01545-010.1007/s10854-019-01545-0 ↗
34. 10.1016/j.ceramint.2020.09.22810.1016/j.ceramint.2020.09.228 ↗
35. 10.1039/C7TA09857J10.1039/C7TA09857J ↗
36. 10.1016/j.cej.2020.12803210.1016/j.cej.2020.128032 ↗