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Polar Properties and Hysteresis Loops in Multilayered Thin Films Ferroelectric/Virtual Ferroelectric

机译:多层薄膜中的极性和磁滞回线   铁电/虚拟铁电

摘要

In the framework of Landau--Ginzburg--Devonshire (LGD) phenomenologicaltheory, the influence of misfit strains, surface energy, and finite-sizeeffects on phase diagrams, polar properties, and hysteresis loops has beencalculated for multilayered thin films of the type ferroelectric/virtualferroelectric. The influence of elastic deformations that arise at theinterface thin film--substrate owing to a mismatch between the latticeconstants in the film and the substrate on the phase diagrams of multilayeredthin films virtual ferroelectric SrTiO$_{3}$/ferroelectric BaTiO$_{3}$ has beenstudied for the first time. In contrast to bulk BaTiO$_{3}$, in which only fourphases (cubic, tetragonal, orthorhombic, and rhombohedral) can exist, it turnedout that six thermodynamically stable BaTiO$_{3}$ phases (paraelectric phaseand tetragonal (FEc), two monoclinic (FEaac and FEac), and two orthorhombic(FEa and FEaa) ferroelectric phases) can exist in multilayeredSrTiO$_{3}$/BaTiO$_{3}$ films. The main polar properties of hysteresis loops(shape, coercive field, and spontaneous polarization) in thin multilayeredSrTiO$_{3}$/BaTiO$_{3}$ films are calculated. It is shown that the systemdemonstrates a strong dependence of its polar properties on the thickness ofSrTiO$_{3}$ and BaTiO$_{3}$ layers, as well as on the elastic misfit strains,with SrTiO$_{3}$ playing the role of dielectric layer: the thicker the layer,the stronger is the depolarization field, which, in its turn, reduces thespontaneous polarization in the BaTiO$_{3}$ film.
机译:在Landau-Ginzburg-Devonshire(LGD)现象学理论的框架内,已经计算了铁电/多层薄膜的失配应变,表面能和有限尺寸效应对相图,极性性质和磁滞回线的影响。虚拟铁电。由于薄膜中的晶格常数和基板之间的晶格常数不匹配,在界面薄膜-基板上产生的弹性变形对多层薄膜的相图的影响:虚拟铁电SrTiO $ _ {3} $ /铁电BaTiO $ _ {3 } $已被首次研究。与仅存在四个相(立方,四方,正交,菱面体)的块状BaTiO $ _ {3} $相比,事实证明六个热力学稳定的BaTiO $ _ {3} $相(顺电相和四方相(FEc)) ,SrTiO $ _ {3} $ / BaTiO $ _ {3} $多层膜中可以存在两个单斜晶(FEaac和FEac)和两个正交晶(FEa和FEaa)铁电相。计算了多层SrTiO $ _ {3} $ / BaTiO $ _ {3} $薄膜的磁滞回线的主要极性(形状,矫顽场和自发极化)。结果表明,该体系证明了其极性性质对SrTiO $ _ {3} $和BaTiO $ _ {3} $层的厚度以及弹性失配应变的强烈依赖性,其中SrTiO $ _ {3} $起到介电层的作用:层越厚,去极化场越强,这反过来又降低了BaTiO $ _ {3} $膜的自发极化。

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