Phonons from density-functional perturbation theory using the all-electron full-potential linearized augmented plane-wave method FLEUR * * Dedicated to the memory of Henry Krakauer (1947–2023).

IF 2.9 Q3 CHEMISTRY, PHYSICAL Electronic Structure Pub Date : 2024-01-04 DOI:10.1088/2516-1075/ad1614
Christian-Roman Gerhorst, Alexander Neukirchen, Daniel A Klüppelberg, Gustav Bihlmayer, Markus Betzinger, Gregor Michalicek, Daniel Wortmann, Stefan Blügel
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Abstract

Phonons are quantized vibrations of a crystal lattice that play a crucial role in understanding many properties of solids. Density functional theory provides a state-of-the-art computational approach to lattice vibrations from first-principles. We present a successful software implementation for calculating phonons in the harmonic approximation, employing density-functional perturbation theory within the framework of the full-potential linearized augmented plane-wave method as implemented in the electronic structure package FLEUR. The implementation, which involves the Sternheimer equation for the linear response of the wave function, charge density, and potential with respect to infinitesimal atomic displacements, as well as the setup of the dynamical matrix, is presented and the specifics due to the muffin-tin sphere centered linearized augmented plane-wave basis-set and the all-electron nature are discussed. As a test, we calculate the phonon dispersion of several solids including an insulator, a semiconductor as well as several metals. The latter are comprised of magnetic, simple, and transition metals. The results are validated on the basis of phonon dispersions calculated using the finite displacement approach in conjunction with the FLEUR code and the phonopy package, as well as by some experimental results. An excellent agreement is obtained.
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使用全电子全电位线性化增强平面波方法的密度函数扰动理论中的声子 FLEUR * * 献给亨利-克拉考尔(Henry Krakauer,1947-2023 年)。
声子是晶体晶格的量子化振动,在理解固体的许多特性方面起着至关重要的作用。密度泛函理论从第一原理出发,为晶格振动提供了最先进的计算方法。我们在电子结构软件包 FLEUR 中实施的全电位线性化增强平面波方法框架内,采用密度泛函扰动理论,成功地实现了谐波近似中的声子计算。该方法的实现涉及波函数、电荷密度和电势相对于无限小原子位移的线性响应的斯特恩海默方程,以及动力学矩阵的设置。作为测试,我们计算了几种固体的声子色散,包括一种绝缘体、一种半导体和几种金属。后者包括磁性金属、简单金属和过渡金属。计算结果以结合 FLEUR 代码和声谱软件包使用有限位移方法计算的声子色散为基础,并通过一些实验结果进行了验证。结果非常吻合。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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CiteScore
3.70
自引率
11.50%
发文量
46
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