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含杂质的球形偶极子铁电玻璃:极性纳米区域、对外加电场的响应及遍历性破坏

Ferroelectric glass of spheroidal dipoles with impurities: polar nanoregions, response to applied electric field, and ergodicity breakdown.

作者信息

Takae Kyohei, Onuki Akira

机构信息

Institute of Industrial Science, University of Tokyo, 4-6-1 Komaba, Meguro-ku, Tokyo 153-8505, Japan.

出版信息

J Phys Condens Matter. 2017 Apr 26;29(16):165401. doi: 10.1088/1361-648X/aa6184. Epub 2017 Feb 20.

Abstract

Using molecular dynamics simulation, we study dipolar glass in crystals composed of slightly spheroidal, polar particles and spherical, apolar impurities between metal walls. We present physical pictures of ferroelectric glass, which have been observed in relaxors, mixed crystals (such as KCN KBr ), and polymers. Our systems undergo a diffuse transition in a wide temperature range, where we visualize polar nanoregions (PNRs) surrounded by impurities. In our simulation, the impurities form clusters and their space distribution is heterogeneous. The polarization fluctuations are enhanced at relatively high T depending on the size of the dipole moment. They then form frozen PNRs as T is further lowered into the nonergodic regime. As a result, the dielectric permittivity exhibits the characteristic features of relaxor ferroelectrics. We also examine nonlinear response to cyclic applied electric field and nonergodic response to cyclic temperature changes (ZFC/FC), where the polarization and the strain change collectively and heterogeneously. We also study antiferroelectric glass arising from molecular shape asymmetry. We use an Ewald scheme of calculating the dipolar interaction in applied electric field.

摘要

利用分子动力学模拟,我们研究了由略微椭球形的极性粒子和金属壁之间的球形非极性杂质组成的晶体中的偶极玻璃。我们展示了在弛豫铁电体、混合晶体(如KCN - KBr)和聚合物中观察到的铁电玻璃的物理图像。我们的系统在很宽的温度范围内经历漫散转变,在此过程中我们观察到被杂质包围的极性纳米区域(PNR)。在我们的模拟中,杂质形成团簇,其空间分布是不均匀的。在相对较高的温度下,极化涨落会根据偶极矩的大小而增强。随着温度进一步降低到非遍历区域,它们会形成冻结的PNR。结果,介电常数呈现出弛豫铁电体的特征。我们还研究了对循环施加电场的非线性响应以及对循环温度变化(零场冷却/场冷,ZFC/FC)的非遍历响应,其中极化和应变会共同且非均匀地变化。我们还研究了由分子形状不对称引起的反铁电玻璃。我们使用埃瓦尔德方法来计算外加电场中的偶极相互作用。

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