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Systematic ab initio study of the phase diagram of epitaxially strained SrTiO_3

机译:外延拉伸SrTiO_3相图的系统从头算研究

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We use density-functional theory with the local-density approximation to study the structural and ferroelectric properties of SrTiO_3 under misfit strains. Both the antiferrodistortive (AFD) and ferroelectric (FE) instabilities are considered by calculating all the phases predicted by Pertsev et al. [Phys. Rev. B 61, R825 (2000)] based on the phenomenological Landau theory. The rotation of the oxygen octahedra and the movement of the atoms are fully relaxed within the constraint of a fixed in-plane lattice constant. We find a rich misfit strain induced phase transition sequence which is in overall agreement with the prediction by Pertsev et al. and is obtained only when the AFD distortion is taken into account. Nevertheless, the calculated locations of the phase boundaries are different from the prediction by Pertsev et al. We also find that compressive misfit strains induce ferroelectricity in the tetragonal low temperature phase only while tensile strains induce ferroelectricity in the orthorhombic phases only. The calculated FE polarization for both the tetragonal and orthorhombic phases increases monotonically with the magnitude of the strains. The AFD rotation angle of the oxygen octahedra in the tetragonal phase increases dramatically as the misfit strain goes from the tensile to compressive strain region while it decreases slightly in the orthorhombic (FO4) phase. This reveals why the polarization in the epitaxially strained SrTiO_3 would be larger when the tensile strain is applied, since the AFD distortion is found to reduce the FE instability and even to completely suppress it in the small strain region. Finally, our analysis of the average polar distortion and the charge density distribution suggests that both the Ti-O and Sr-O layers contribute significantly to the FE polarization.
机译:我们使用密度泛函理论与局部密度近似来研究失配应变下SrTiO_3的结构和铁电性能。反铁变形(AFD)和铁电(FE)的不稳定性都通过计算Pertsev等人预测的所有相位来考虑。 [物理B 61,R825(2000)]基于现象学的朗道理论。在固定的面内晶格常数的约束下,氧八面体的旋转和原子的运动被完全放松。我们发现一个丰富的失配应变引起的相变序列,与Pertsev等人的预测总体上是一致的。并且只有在考虑到AFD失真时才能获得。然而,相界的计算位置与Pertsev等人的预测不同。我们还发现,压缩失配应变仅在四方低温相中感应铁电,而拉伸应变仅在正交相中感应铁电。正交相和正交相的计算出的FE极化随应变的大小单调增加。氧八面体在四方相中的AFD旋转角度随着失配应变从拉伸应变区域进入压缩应变区域而急剧增加,而在正交晶(FO4)相中则略有减小。这揭示了为什么在施加拉伸应变时外延应变的SrTiO_3中的极化会更大,因为发现AFD畸变可以减小FE的不稳定性,甚至可以在小应变区域完全抑制它的不稳定性。最后,我们对平均极性畸变和电荷密度分布的分析表明,Ti-O和Sr-O层均对FE极化起重要作用。

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