论文标题
材料的非harm谐度量
Anharmonicity Measure for Materials
论文作者
论文摘要
用于定性和定量描述固体中的核动力学的理论框架通常基于谐波近似。但是,已知这种近似值在许多现代功能材料中变得不准确或完全分解。有趣的是,到目前为止,还没有可靠的措施来量化非谐调。因此,目前不可能根据非谐调性和方法的系统分类和方法的基准,而方法可能是适合非谐音优势的方法。在这项工作中,我们得出并讨论了一项统计措施,该统计措施可通过“非谐度程度”可靠地对跨温度制度和材料类别进行分类。这使我们能够区分“谐波”材料,对谐波效应构成了谐波近似之上的微小扰动,即强烈的“非谐”材料,对于这种材料而言,对此,非谐作效应变得很重要甚至显着,并且在扰动理论方面对非谐度的治疗却远远超出了问题。我们表明,在真实和相互空间中对该度量的分析也能够阐明基本的微观机制,即使在接近(例如,相变或缺陷形成)的条件下也是如此。最终,我们证明了开发的方法是计算上有效的,并通过对数百个二元固体进行扫描来实现快速的高通量搜索。结果表明,超出扰动极限以外的强大无谐作用不仅在复杂的材料中或接近相变的活性,而且已经在简单的二元化合物中处于中等温度。
Theoretical frameworks used to qualitatively and quantitatively describe nuclear dynamics in solids are often based on the harmonic approximation. However, this approximation is known to become inaccurate or to break down completely in many modern functional materials. Interestingly, there is no reliable measure to quantify anharmonicity so far. Thus, a systematic classification of materials in terms of anharmonicity and a benchmark of methodologies that may be appropriate for different strengths of anharmonicity is currently impossible. In this work, we derive and discuss a statistical measure that reliably classifies compounds across temperature regimes and material classes by their "degree of anharmonicity". This enables us to distinguish "harmonic" materials, for which anharmonic effects constitute a small perturbation on top of the harmonic approximation, from strongly "anharmonic" materials, for which anharmonic effects become significant or even dominant and the treatment of anharmonicity in terms of perturbation theory is more than questionable. We show that the analysis of this measure in real and reciprocal space is able to shed light on the underlying microscopic mechanisms, even at conditions close to, e.g., phase transitions or defect formation. Eventually, we demonstrate that the developed approach is computationally efficient and enables rapid high-throughput searches by scanning over a set of several hundred binary solids. The results show that strong anharmonic effects beyond the perturbative limit are not only active in complex materials or close to phase transitions, but already at moderate temperatures in simple binary compounds.