Theoretical Sciences Unit and Sheikh Saqr Laboratory, J Nehru Centre for Advanced Scientific Research , Jakkur PO, Bangalore 560 064 India.
Acc Chem Res. 2014 Nov 18;47(11):3242-9. doi: 10.1021/ar500331c. Epub 2014 Oct 31.
A ferroelectric crystal exhibits macroscopic electric dipole or polarization arising from spontaneous ordering of its atomic-scale dipoles that breaks inversion symmetry. Changes in applied pressure or electric field generate changes in electric polarization in a ferroelectric, defining its piezoelectric and dielectric properties, respectively, which make it useful as an electromechanical sensor and actuator in a number of applications. In addition, a characteristic of a ferroelectric is the presence of domains or states with different symmetry equivalent orientations of spontaneous polarization that are switchable with large enough applied electric field, a nonlinear property that makes it useful for applications in nonvolatile memory devices. Central to these properties of a ferroelectric are the phase transitions it undergoes as a function of temperature that involve lowering of the symmetry of its high temperature centrosymmetric paraelectric phase. Ferroelectricity arises from a delicate balance between short and long-range interatomic interactions, and hence the resulting properties are quite sensitive to chemistry, strains, and electric charges associated with its interface with substrate and electrodes. First-principles density functional theoretical (DFT) calculations have been very effective in capturing this and predicting material and environment specific properties of ferroelectrics, leading to fundamental insights into origins of ferroelectricity in oxides and chalcogenides uncovering a precise picture of electronic hybridization, topology, and mechanisms. However, use of DFT in molecular dynamics for detailed prediction of ferroelectric phase transitions and associated temperature dependent properties has been limited due to large length and time scales of the processes involved. To this end, it is quite appealing to start with input from DFT calculations and construct material-specific models that are realistic yet simple for use in large-scale simulations while capturing the relevant microscopic interactions quantitatively. In this Account, we first summarize the insights obtained into chemical mechanisms of ferroelectricity using first-principles DFT calculations. We then discuss the principles of construction of first-principles model Hamiltonians for ferroelectric phase transitions in perovskite oxides, which involve coarse-graining in time domain by integrating out high frequency phonons. Molecular dynamics simulations of the resulting model are shown to give quantitative predictions of material-specific ferroelectric transition behavior in bulk as well as nanoscale ferroelectric structures. A free energy landscape obtained through coarse-graining in real-space provides deeper understanding of ferroelectric transitions, domains, and states with inhomogeneous order and points out the key role of microscopic coupling between phonons and strain. We conclude with a discussion of the multiscale modeling strategy elucidated here and its application to other materials such as shape memory alloys.
铁电晶体表现出宏观电偶极或极化,这是由于其原子级偶极子的自发有序排列而产生的,这种有序排列打破了反转对称。施加的压力或电场的变化会在铁电体中产生电极化的变化,分别定义其压电和介电特性,这使其成为许多应用中机电传感器和执行器的有用材料。此外,铁电体的一个特征是存在具有不同对称等效自发极化取向的畴或状态,这些状态可以通过足够大的外加电场进行切换,这是非线性特性,使其在非易失性存储器件的应用中很有用。铁电体的这些特性的核心是其随温度经历的相变,这涉及到其高温中心对称顺电相的对称降低。铁电性源于短程和长程原子间相互作用之间的微妙平衡,因此,由此产生的性质对其与衬底和电极的界面相关的化学、应变和电荷非常敏感。第一性原理密度泛函理论(DFT)计算在捕捉这一点和预测铁电体的材料和环境特性方面非常有效,从而深入了解氧化物和硫属化物中铁电性的起源,揭示了电子杂化、拓扑和机制的精确图景。然而,由于涉及的过程的长度和时间尺度较大,DFT 在分子动力学中用于详细预测铁电相变和相关温度依赖特性的应用受到限制。为此,从 DFT 计算开始并构建针对特定材料的模型非常有吸引力,这些模型既现实又简单,可用于大规模模拟,同时定量捕捉相关的微观相互作用。在本报告中,我们首先总结了使用第一性原理 DFT 计算获得的关于铁电性化学机制的见解。然后,我们讨论了钙钛矿氧化物中铁电相变的第一性原理模型哈密顿量的构建原理,该原理涉及通过整合高频声子在时域中的粗粒化。结果表明,对所得模型的分子动力学模拟可以对块状和纳米级铁电结构中的材料特定铁电转变行为进行定量预测。通过实空间粗粒化获得的自由能景观提供了对铁电转变、畴和具有非均匀有序的状态的更深入理解,并指出了声子和应变之间微观耦合的关键作用。最后,我们讨论了这里阐明的多尺度建模策略及其在其他材料(如形状记忆合金)中的应用。