Electric-field-induced antiferroelectric to ferroelectric phase transition in hot-pressed PbZrO3
Source abstract
Abstract
Double polarization hysteresis loops associated with field-induced antiferroelectric-ferroelectric (AFE-FE) phase transitions, which underpin many antiferroelectric functionalities, are rarely observed in PbZrO 3 polycrystals at ambient conditions because the required critical field often approaches the dielectric breakdown strength. Here, dense PbZrO 3 ceramics fabricated by hot pressing reach 97.8% relative density and exhibit an orthorhombic Pbam average structure, as confirmed by high-energy X-ray diffraction. A sharp paraelectric-antiferroelectric anomaly is observed at 235 °C, with a peak permittivity of 5387 at 10 kHz and negligible frequency dispersion. Room-temperature polarization measurements demonstrate a field-induced AFE-FE transition can be triggered at 27 kV/mm, yielding well-defined double hysteresis loops with forward and backward critical fields of 26.5 kV/mm and 19.1 kV/mm, respectively. The ceramics deliver a recoverable energy density of 3.6 J/cm 3 with an efficiency of 73.5%, accompanied by a large field-induced strain of 0.49%. Large-signal dielectric measurement reveals a non-monotonic field dependence of permittivity, featuring a pronounced enhancement as the forward transition is approached. Atomistic-resolution electron microscopy and polarization mapping directly resolve the commensurately modulated antipolar “↑↑↓↓” order and quantify an average Pb displacement of ∼24 pm with dipoles aligned along <110> directions. These results establish a room-temperature experimental benchmark for pristine bulk PbZrO 3 , linking atomistic-scale antipolar order to macroscopic transition and providing a quantitative baseline for evaluating phase competition and transition pathways in antiferroelectric perovskites. • Room-temperature AFE-FE transition is clearly shown in bulk polycrystals, yielding double hysteresis loops at 27 kV/mm. • Quantitative benchmarks set: E F =26.5 kV/mm, E B =19.1 kV/mm, W rec =3.6 J/cm 3 , η =73.5%, and field-induced strain =0.49%.. • STEM mapping resolves “↑↑↓↓” order, ∼24 pm Pb displacement along <110>, linking atomic order to macroscopic switching.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Ferroelectric and Piezoelectric Materials · Ferroelectric and Negative Capacitance Devices · Multiferroics and related materials
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (43)
Show source-provided references
1. Antiferroelectrics: history, fundamentals, crystal chemistry, crystal structures, size effects, and applications10.1111/jace.17834 ↗
2. Antiferroelectrics for energy storage applications: a review10.1002/admt.201800111 ↗
3. Review on field-induced phase transitions in lead-free NaNbO3-based antiferroelectric perovskite oxides for energy storage10.1016/j.jmat.2022.09.008 ↗
4. Dielectric properties of lead zirconate10.1103/PhysRev.84.476 ↗
5. Antiferroelectric structure of lead zirconate10.1103/PhysRev.83.1078 ↗
6. Piezoelectric ceramics with high piezoelectricity and broad temperature usage range10.1016/j.jmat.2020.11.012 ↗
7. Phase transitions in antiferroelectric PbHfO310.1103/PhysRev.91.812 ↗
8. Composition-tailor induced electrocaloric effect near room temperature in (Pb,Ba)HfO3 films10.1016/j.jmat.2022.12.002 ↗
9. Field-forced antiferroelectric-to-ferroelectric switching in modified lead zirconate titanate stannate ceramics10.1111/j.1151-2916.1989.tb06177.x ↗
10. Incommensurately modulated polar structures in antiferroelectric tin-modified lead zirconate titanate: II, dependence of structure-property relations on tin content10.1111/j.1151-2916.1998.tb02616.x ↗
11. Enhanced energy-storage density and temperature stability of Pb0.89La0.06Sr0.05(Zr0.95Ti0.05)O3 anti-ferroelectric thin film capacitor
12. Interplay of conventional with inverse electrocaloric response in (Pb,Nb)(Zr,Sn,Ti)O3 antiferroelectric materials10.1103/PhysRevB.97.094113 ↗
13. Electric-field-induced antiferroelectric to ferroelectric phase transition in mechanically confined Pb0.99Nb0.02[(Zr0.57Sn0.43)0.94Ti0.06]0.98O310.1103/PhysRevB.81.014103 ↗
14. Electric-field-induced antiferroelectric to ferroelectric phase transition in polycrystalline NaNbO310.1016/j.actamat.2020.09.002 ↗
15. Tailoring high-energy storage NaNbO3-based materials from antiferroelectric to relaxor states10.1038/s41467-023-37060-4 ↗
16. Design of lead-free antiferroelectric (1–x)NaNbO3-xSrSnO3 compositions guided by first-principles calculations10.1021/acs.chemmater.0c03685 ↗
17. Lead-free antiferroelectric niobates AgNbO3 and NaNbO3 for energy storage applications10.1039/D0TA08345C ↗
18. Lead-free antiferroelectric silver niobate tantalate with high energy storage performance
19. Energy storage performance and phase transition under high electric field in Na/Ta co-doped AgNbO3 ceramics10.1016/j.jmat.2022.09.007 ↗
20. Order-disorder transition in the prototypical antiferroelectric PbZrO310.1103/PhysRevB.100.020102 ↗
21. Structure and disorder in single-crystal lead zirconate, PbZrO3
22. Crystal structure determination of antiferroelectric PbZrO3-application of profile analysis method to powder method of X-ray and neutron diffraction10.1143/JPSJ.51.3583 ↗
23. On the possibility that PbZrO3 not be antiferroelectric10.1038/s41524-021-00671-w ↗
24. A re-examination of antiferroelectric PbZrO3 and PbHfO3 : an 80-atom Pnam structure
25. Phase transitions and spontaneous polarization in PbZrO310.1002/pssa.2210280213 ↗
26. Preparation of highly dense PZN-PZT thick films by the aerosol deposition method using Excess-PbO powder10.1111/j.1551-2916.2007.01901.x ↗
27. Overview of SSRF phase-II beamlines10.1007/s41365-024-01487-1 ↗
28. Ultrahard X-ray multifunctional application beamline at the SSRF10.1007/s41365-024-01468-4 ↗
29. EXPGUI, a graphical user interface for GSAS10.1107/S0021889801002242 ↗
30. DIOPTAS: a program for reduction of two-dimensional X-ray diffraction data and data exploration10.1080/08957959.2015.1059835 ↗
31. StatSTEM: an efficient approach for accurate and precise model-based quantification of atomic resolution electron microscopy images10.1016/j.ultramic.2016.08.018 ↗
32. Advanced electron crystallography through model-based imaging10.1107/S2052252515019727 ↗
33. Superstructure determination of PbZrO3
34. Dielectric properties of oriented thin films of PbZrO3 on Si produced by pulsed laser ablation10.1063/1.367955 ↗
35. The structural phase transitions in lead zirconate in super-high electric fields10.1080/00150197808237203 ↗
36. Understanding the effects of electric-field-induced phase transition and polarization loop behavior on the energy storage performance of antiferroelectric PbZrO3 thin films10.1016/j.tsf.2020.137794 ↗
37. Hardening effect in lead-free piezoelectric ceramics10.1557/s43578-020-00016-1 ↗
38. Sodium lithium niobate lead-free piezoceramics for high-power applications: fundamental, progress, and perspective
39. Life cycle assessment of lead-free potassium sodium niobate versus lead zirconate titanate: energy and environmental impacts10.1002/eom2.12450 ↗
40. Revealing the mechanism of electric-field-induced phase transition in antiferroelectric NaNbO3 by in situ high-energy X-ray diffraction10.1063/5.0043050 ↗
41. Antiferroelectric structure of lead zirconate10.1103/PhysRev.83.1078 ↗
42. The origin of antiferroelectricity in PbZrO310.1038/ncomms3229 ↗
43. Unveiling the ferrielectric nature of PbZrO3-based antiferroelectric materials10.1038/s41467-020-17664-w ↗