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Energy storage and dielectric properties in PbZrO3/PbZrTiO3 antiferroelectric/ferroelectric bilayer bulk structure using Landau theory.

Authors :
Alrub, Ahmad Musleh
Anbar, Abd Aljabar
Ibrahim, Abdel-Baset M. A.
Source :
AIP Advances; Jun2024, Vol. 14 Issue 6, p1-9, 9p
Publication Year :
2024

Abstract

Employing Landau theory and the Landau–Khalatnikov (L–K) equation of motion, we investigate the phase transitions in individual layers of antiferroelectric lead zirconate (PbZrO<subscript>3</subscript>), ferroelectric lead zirconate titanate (PbZrTiO<subscript>3</subscript>), and an antiferroelectric/ferroelectric PbZrO<subscript>3</subscript>/PbZr<subscript>(0.21)</subscript>Ti<subscript>(0.79)</subscript>O<subscript>3</subscript> bilayer bulk structure. We examine the dielectric hysteresis loop behavior of the three systems, with a specific focus on the PbZrO<subscript>3</subscript>/PbZr<subscript>(0.21)</subscript>Ti<subscript>(0.79)</subscript>O<subscript>3</subscript> bilayer under different stabilities of the PbZrO<subscript>3</subscript> layer. In addition, we explore cases where the coercive field of the bilayer structure is lower than that of the PbZrTiO<subscript>3</subscript> individual layer. The recoverable electric energy for the PbZrO<subscript>3</subscript>/PbZr<subscript>(0.21)</subscript>Ti<subscript>(0.79)</subscript>O<subscript>3</subscript> bilayer increases significantly to 118 J/cm<superscript>3</superscript> at an applied field of 7.5 × 10<superscript>8</superscript> V/m at 20 °C. In comparison, the PbZr<subscript>(0.21)</subscript>Ti<subscript>(0.79)</subscript>O<subscript>3</subscript> layer reaches 71.8 J/cm<superscript>3</superscript> under the same field and temperature conditions. This is much higher than those predicted experimentally by previous studies on thin film single and bilayer structures (15.6 and 28.2 J/Cm<superscript>3</superscript> respectively), indicating that the antiferroelectric/ferroelectric PbZrO<subscript>3</subscript>/PbZr<subscript>(0.21)</subscript>Ti<subscript>(0.79)</subscript>O<subscript>3</subscript> bilayer bulk structure could be used to target specific large-scale, long-term energy storage applications. Upon increasing the value of the coupling coefficient, the transition temperatures of the PbZrO<subscript>3</subscript> layer and the PbZrO<subscript>3</subscript>/PbZr<subscript>(0.21)</subscript>Ti<subscript>(0.79)</subscript>O<subscript>3</subscript> bilayer are increased up to the transition temperature of the PbZr<subscript>(0.21)</subscript>Ti<subscript>(0.79)</subscript>O<subscript>3</subscript> individual layer (450 °C). This increment in the transition temperature in the bilayer system contributes to its stability in storing energy at higher temperatures. Furthermore, the recoverable energy density of the PbZrO<subscript>3</subscript>/PbZr<subscript>(0.21)</subscript>Ti<subscript>(0.79)</subscript>O<subscript>3</subscript> bilayer increases further with temperature from 20 to 440 °C correlated with the rise in the difference between the spontaneous and the remanent polarizations (P<subscript>s</subscript> − P<subscript>r</subscript>). The significant stored energy observed over a wide temperature range highlights the promise of this bilayer structure for creating high-power capacitors where stability at different temperatures is crucial and possesses greater energy storage capacity. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
21583226
Volume :
14
Issue :
6
Database :
Complementary Index
Journal :
AIP Advances
Publication Type :
Academic Journal
Accession number :
178147880
Full Text :
https://doi.org/10.1063/5.0200797