The evolution of anti-vortex like domain under electric field in polycrystalline ferroelectric

被引:1
|
作者
Tian, Xiaobao [1 ,2 ]
Zhou, Changchun [3 ]
He, Xiaoqiao [2 ,4 ]
Zhou, Zhihong [1 ]
Chen, Yu [1 ]
Guo, Hao [1 ]
Fan, Haidong [1 ]
机构
[1] Sichuan Univ, Dept Mech, Chengdu 610065, Sichuan, Peoples R China
[2] City Univ Hong Kong, Dept Architecture & Civil Engn, Tat Chee Ave, Hong Kong, Hong Kong, Peoples R China
[3] Sichuan Univ, Natl Engn Res Ctr Biomat, Chengdu 610064, Peoples R China
[4] City Univ Hong Kong, Shenzhen Res Inst, Ctr Adv Struct Mat, Shenzhen 518057, Peoples R China
基金
中国国家自然科学基金;
关键词
Polycrystalline ferroelectric; Anti-vortex; Motion; Electric field; HEAT-TRANSFER; NANOFLUID FLOW; SIMULATION; ANNIHILATION; CONVECTION; RADIATION;
D O I
10.1016/j.compositesb.2018.07.063
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Domain wall (DW) plays an important role in the domain evolution. The anti-vortex could be a special domain structure of the mixed DWs, i.e. the Ising wall and the Mixed Ising-Neel wall. The anti-vortex domain in polycrystalline ferroelectric has been investigated by a modified first-principles-based atomistic method incorporating the anisotropic shell model. Results show that the nucleation and the disappearance of the anti-vortex happen at grain boundaries (GBs) under sinusoidal electric fields loading. As the anti-vortex motion by the electric field, it is a perfect view point for the domain evolutions. It has been found that the anti-vortex core can't pass through the GBs because of the size and disorder field. This phenomenon indicates that anti-vortex is only been obtained in grains at polycrystalline ferroelectric, and the electric field range must between -6.3 and 6.3 x 10(8) V/m.
引用
收藏
页码:195 / 199
页数:5
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