Physics Department and Institute for Nanoscience and Engineering, University of Arkansas, Fayetteville, Arkansas 72701, USA and Physics Department and Institute of Physics, South Federal University, Rostov-on-Don 344090, Russia.
Electronic Materials Research Laboratory, Key Laboratory of the Ministry of Education and International Center for Dielectric Research, Xi'an Jiaotong University, Xi'an 710049, China.
Phys Rev Lett. 2013 Dec 13;111(24):247602. doi: 10.1103/PhysRevLett.111.247602. Epub 2013 Dec 10.
Finite-temperature properties of epitaxial films made of Ba(Zr,Ti)O3 relaxor ferroelectrics are determined as a function of misfit strain, via the use of a first-principles-based effective Hamiltonian. These films are macroscopically paraelectric at any temperature, for any strain ranging between ≃-3% and ≃+3%. However, original temperature-versus-misfit strain phase diagrams are obtained for the Burns temperature (Tb) and for the critical temperatures (Tm,z and Tm,IP) at which the out-of-plane and in-plane dielectric response peak, respectively, which allow the identification of three different regions. These latter differ from their evolution of Tb, Tm,z, and/or Tm,IP with strain, which are the fingerprints of a remarkable strain-induced microscopic change: each of these regions is associated with its own characteristic behavior of polar nanoregions at low temperature, such as strain-induced rotation or strain-driven elongation of their dipoles or even increase in the average size of the polar nanoregions when the strength of the strain grows.
通过使用基于第一性原理的有效哈密顿量,我们确定了外延薄膜的有限温度性质,外延薄膜由 Ba(Zr,Ti)O3 弛豫铁电体制成,其功能取决于失配应变。对于任何应变范围在 ≃-3% 到 ≃+3% 之间的应变,这些薄膜在任何温度下都是宏观的顺电体。然而,对于 Burns 温度 (Tb) 和临界温度 (Tm,z 和 Tm,IP),我们得到了原始的温度-失配应变相图,分别对应于体和面内介电响应的峰值,这允许识别三个不同的区域。这些区域与 Tb、Tm,z 和/或 Tm,IP 随应变的演变不同,这是微观应变诱导变化的显著特征:每个区域都与低温下的极性纳米区域的特有行为相关,例如应变诱导的极性纳米区域的旋转或应变驱动的其偶极子的伸长,甚至当应变强度增加时平均尺寸增加。