Electric-field-induced dipole reorientation characteristics in paraelectric KTN crystals

B Bohan Xing (School of Physics, Harbin Institute of Technology 1 , Harbin 150001,) M Minghui Cao (Department of Pathology, University of California, San Diego, La Jolla, California 92093, United States) X Xiangda Meng (School of Physics, Harbin Institute of Technology 1 , Harbin 150001,) Y Yu Wang X Xing Wen (New Cornerstone Science Laboratory, Department of Biology, School of Life Sciences, Institute of Plant and Food Science, Southern University of Science and Technology) X Xinyu Jin (School of Physics, Harbin Institute of Technology 1 , Harbin 150001,) J Jinyu Ruan (School of Physics, Harbin Institute of Technology 1 , Harbin 150001,) C Chengpeng Hu (School of Physics, Harbin Institute of Technology 1 , Harbin 150001,) Q Qingxin Meng P Peng Tan H Hao Tian (Shanghai Research Institute of Petrochemical Technology)

Abstract

Local dipoles significantly influence the properties of paraelectric perovskites. Potassium tantalate niobate (KTa1−xNbxO3, abbreviated as KTN) is a perovskite with excellent electro-optic and piezoelectric properties. Manipulating dipoles via electric fields in paraelectric KTN demonstrates significant application potential. Therefore, such dipole dynamics under electric fields are essential to research. In this work, we investigated dipole reorientation under electric fields in paraelectric KTN crystals. We found that, under an electric field of 10 kV/cm, local polarization opposing the direction of the applied field still exists in the KTa0.62Nb0.38O3 (TC = 13 °C) crystal. Additionally, a macroscopic piezoelectric coefficient of ∼40 pC/N was achieved in the paraelectric KTa0.62Nb0.38O3 crystal by applying a 12.5 kV/cm electric field for 24 h. This phenomenon is attributed to the maintainable field-induced reorientation state of the dipoles after the removal of the electric field. Furthermore, since complete dipole reorientation requires strong fields, in the case of a KTa0.61Nb0.39O3 crystal with a TC (23 °C) approaching room temperature, a field-induced phase transition (at 2.1 kV/cm) occurs prior to the complete switching of dipoles in the paraelectric phase. This results in a multi-domain state in the recently phase-transformed crystal. Our findings help in understanding the performance exhibited under electric fields and can facilitate the optimization of paraelectric perovskites.

Article Details

Volume / Issue Vol. 127, Issue 10
Published September 08, 2025
ISSN 0003-6951
Publisher American Institute of Physics

Journal Info

Applied Physics Letters

American Institute of Physics

ISSN: 0003-6951 Physical Sciences

Authors (11)

B

Bohan Xing

School of Physics, Harbin Institute of Technology 1 , Harbin 150001,

M

Minghui Cao

Department of Pathology, University of California, San Diego, La Jolla, California 92093, United States

X

Xiangda Meng

School of Physics, Harbin Institute of Technology 1 , Harbin 150001,

Y

Yu Wang

X

Xing Wen

New Cornerstone Science Laboratory, Department of Biology, School of Life Sciences, Institute of Plant and Food Science, Southern University of Science and Technology

X

Xinyu Jin

School of Physics, Harbin Institute of Technology 1 , Harbin 150001,

J

Jinyu Ruan

School of Physics, Harbin Institute of Technology 1 , Harbin 150001,

C

Chengpeng Hu

School of Physics, Harbin Institute of Technology 1 , Harbin 150001,

Q

Qingxin Meng

P

Peng Tan

H

Hao Tian

Shanghai Research Institute of Petrochemical Technology