Phase transition behavior in ferroelectric BaTi0.8Zr0.2O3: Evidence of polar cluster reorientation above Curie temperature

O Oktay Aktas (State Key Laboratory for Mechanical Behavior of Materials and Materials Science and Engineering, Xi'an Jiaotong University 1 , Xi'an 710049,) F Francisco Javier Romero (Departamento de Física de la Materia Condensada, ICMSE-CSIC, Universidad de Sevilla 3 , Apartado 1065, Sevilla 41080,) Z Zhengwang He (State Key Laboratory for Mechanical Behavior of Materials and Materials Science and Engineering, Xi'an Jiaotong University 1 , Xi'an 710049,) G Gan Linyu (State Key Laboratory for Mechanical Behavior of Materials & Materials Science and Engineering, Xi’an Jiaotong University 1 , Xi’an 710049,) X Xiangdong Ding J José-María Martín-Olalla (Departamento de Física de la Materia Condensada, ICMSE-CSIC, Universidad de Sevilla 3 , Apartado 1065, Sevilla 41080,) M María-Carmen Gallardo (Departamento de Física de la Materia Condensada, ICMSE-CSIC, Universidad de Sevilla 3 , Apartado 1065, Sevilla 41080,) T Turab Lookman (State Key Laboratory for Mechanical Behavior of Materials, School of Materials Science and Engineering, Xi’an Jiaotong University 1 , Xi’an 710049,)

Abstract

We study the phase transition behavior of the ferroelectric BaTi0.8Zr0.2O3 in the paraelectric region above the Curie temperature. The investigation of the phase transition using caloric, dielectric, and elastic measurements indicates that the ferroelectric transition at Tc = 292 K is continuous and displays weakly relaxor characteristics. The nonlinear scaling of entropy and polarization, as well as the temperature dependencies of dielectric and elastic properties, indicates the presence of local structures in the paraelectric phase. The non-zero remnant polarization is measured up to a characteristic temperature T* ∼ 350 K. This temperature coincides with the temperature where the dielectric constant deviates from the Curie–Weiss law and is identified as the coherence temperature T*, associated with the formation of static polar nanostructures. Finally, direct current field cooling in the paraelectric phase using fields smaller than the coercive field leads to an elastic response and remnant piezoelectricity below T*, attributed to the re-orientation of polar nanostructures. The observed remnant effect, along with the temperature dependence of the piezoelectric effect and its time dependence below and above T*, is consistent with increased coherence and slower dynamics of these structures on cooling, leading to symmetry-disallowed remnant piezoelectricity due to glassy behavior below T*.

Article Details

Volume / Issue Vol. 137, Issue 20
Published May 28, 2025
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (8)

O

Oktay Aktas

State Key Laboratory for Mechanical Behavior of Materials and Materials Science and Engineering, Xi'an Jiaotong University 1 , Xi'an 710049,

F

Francisco Javier Romero

Departamento de Física de la Materia Condensada, ICMSE-CSIC, Universidad de Sevilla 3 , Apartado 1065, Sevilla 41080,

Z

Zhengwang He

State Key Laboratory for Mechanical Behavior of Materials and Materials Science and Engineering, Xi'an Jiaotong University 1 , Xi'an 710049,

G

Gan Linyu

State Key Laboratory for Mechanical Behavior of Materials & Materials Science and Engineering, Xi’an Jiaotong University 1 , Xi’an 710049,

X

Xiangdong Ding

J

José-María Martín-Olalla

Departamento de Física de la Materia Condensada, ICMSE-CSIC, Universidad de Sevilla 3 , Apartado 1065, Sevilla 41080,

M

María-Carmen Gallardo

Departamento de Física de la Materia Condensada, ICMSE-CSIC, Universidad de Sevilla 3 , Apartado 1065, Sevilla 41080,

T

Turab Lookman

State Key Laboratory for Mechanical Behavior of Materials, School of Materials Science and Engineering, Xi’an Jiaotong University 1 , Xi’an 710049,