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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >Shear-strain gradient induced polarization reversal in ferroelectric BaTiO_3 thin films: A first-principles total-energy study
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Shear-strain gradient induced polarization reversal in ferroelectric BaTiO_3 thin films: A first-principles total-energy study

机译:剪切应变梯度引起的铁电BaTiO_3薄膜的极化反转:第一性原理全能研究

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摘要

Based on the first-principles total-energy calculation, we have studied the shear-strain gradient effect on the polarization reversal of ferroelectric BaTi03 thin films. By calculating the energies of double-domain supercells for different electric polarization, shear-strain gradients, and domain-wall displacement, we extracted, in addition to the domain-wall energy, the polarization energy, elastic energy, and flexoelectric coefficient of a single domain. The constructed Landau-Devonshire phenomenological theory yields a critical shear-strain gradient of 9.091 × 10~7/m (or a curvature radius (R) of 110 A) for reversing the 180° domain at room temperature, which is on the same order of the experimentally estimated value of 3.333 × 10~7/m (R = 300 A). In contrast to the commonly used linear response theory, the flexoelectric coefficient derived from fitting the total energy to a Landau-Devonshire energy functional does not depend on the specific pseudopotential. Thus, our method offers an alternative numerical approach to study the flexoelectric effect.
机译:基于第一性原理的总能计算,我们研究了剪切应变梯度效应对铁电BaTiO3薄膜极化反转的影响。通过计算不同电极化,剪切应变梯度和畴壁位移的双畴超级电池的能量,除畴壁能量外,我们还提取了单个晶胞的极化能,弹性能和挠电系数域。构造的Landau-Devonshire现象学理论得出的临界剪切应变梯度为9.091×10〜7 / m(或曲率半径(R)为110 A),用于在室温下反转180°域,该阶次相同实验估计值为3.333×10〜7 / m(R = 300 A)。与通常使用的线性响应理论相反,通过将总能量拟合为Landau-Devonshire能量泛函而得出的柔电系数并不取决于特定的伪电势。因此,我们的方法提供了一种替代的数值方法来研究柔电效应。

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  • 来源
    《Physical review. B, Condensed Matter And Materials Physics 》 |2017年第14期| 144111.1-144111.8| 共8页
  • 作者单位

    National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China;

    National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China;

    National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China;

    National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China,Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China;

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