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Influence of dipole defects on polarization switching in the vicinity of a crack in relaxor ferroelectrics

机译:弛豫铁电体中偶极缺陷对裂纹附近极化转换的影响

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Simulations of the polarization switching process near the tip of an edge crack in relaxor ferroelectrics subjected to external electric field have been carried out by employing the time-dependent Ginzburg-Landau theory and the phase-field method. The electric boundary conditions of the crack and the material are assumed to be impermeable and isotropic, respectively. The interaction between dipole defects and the crack and the influence of the dipole defect concentration on the switching process are discussed. The results obtained show that, in relaxor materials, polarization switching in the vicinity of the crack tip is suppressed, and the electric field distribution is not symmetric with respect to the crack surface. These results arise on account of the interaction between dipole defects and the crack and the inhomogeneous electric field induced by dipole defects. Moreover, the polarization switching rate and switching zone area decrease with an increase of dipole defect concentration.View full textDownload full textKeywordsphase-field method, relaxor ferroelectrics, edge crack, polarization switching, dipole defectRelated var addthis_config = { ui_cobrand: "Taylor & Francis Online", services_compact: "citeulike,netvibes,twitter,technorati,delicious,linkedin,facebook,stumbleupon,digg,google,more", pubid: "ra-4dff56cd6bb1830b" }; Add to shortlist Link Permalink http://dx.doi.org/10.1080/09500831003630757
机译:通过采用时变的Ginzburg-Landau理论和相场方法,对松弛铁电体中边缘裂纹尖端附近的极化转换过程进行了仿真。假定裂纹和材料的电边界条件分别是不可渗透的和各向同性的。讨论了偶极缺陷与裂纹之间的相互作用以及偶极缺陷浓度对开关过程的影响。所得结果表明,在弛豫材料中,裂纹尖端附近的极化转换受到抑制,并且电场分布相对于裂纹表面不对称。这些结果是由于偶极缺陷与裂纹之间的相互作用以及偶极缺陷引起的不均匀电场而产生的。而且,极化转换速率和转换区面积随着偶极缺陷浓度的增加而降低。查看全文下载全文关键词相场法,弛豫铁电体,边缘裂纹,极化转换,偶极缺陷相关var addthis_config = {ui_cobrand:“泰勒和弗朗西斯在线”,services_compact:“ citeulike,网络振动,微博,technorati,美味,linkedin,facebook,stumbleupon,digg,google,更多”,发布号:“ ra-4dff56cd6bb1830b”};添加到候选列表链接永久链接http://dx.doi.org/10.1080/09500831003630757

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