Electronic structure calculations with GPAW: a real-space implementation of the projector augmented-wave method

密度泛函理论 基准集 含时密度泛函理论 威恩2K 计算机科学 电子结构 波函数 基础(线性代数) 基函数 原子轨道 投影机 混合功能 计算科学 物理 量子力学 数学 电子 局部密度近似 几何学 计算机视觉
作者
Jussi Enkovaara,C. Rostgaard,J. J. Mortensen,Jun Chen,Marcin Dułak,Lara Ferrighi,Jeppe Gavnholt,Christian Glinsvad,V Haikola,Heine Anton Hansen,Henrik H. Kristoffersen,Mikael Kuisma,Ask Hjorth Larsen,Lauri Lehtovaara,Mathias P. Ljungberg,Olga Lopez‐Acevedo,Poul Georg Moses,Jussi Ojanen,Thomas Olsen,Vivien Petzold
出处
期刊:Journal of Physics: Condensed Matter [IOP Publishing]
卷期号:22 (25): 253202-253202 被引量:2250
标识
DOI:10.1088/0953-8984/22/25/253202
摘要

Electronic structure calculations have become an indispensable tool in many areas of materials science and quantum chemistry. Even though the Kohn-Sham formulation of the density-functional theory (DFT) simplifies the many-body problem significantly, one is still confronted with several numerical challenges. In this article we present the projector augmented-wave (PAW) method as implemented in the GPAW program package (https://wiki.fysik.dtu.dk/gpaw) using a uniform real-space grid representation of the electronic wavefunctions. Compared to more traditional plane wave or localized basis set approaches, real-space grids offer several advantages, most notably good computational scalability and systematic convergence properties. However, as a unique feature GPAW also facilitates a localized atomic-orbital basis set in addition to the grid. The efficient atomic basis set is complementary to the more accurate grid, and the possibility to seamlessly switch between the two representations provides great flexibility. While DFT allows one to study ground state properties, time-dependent density-functional theory (TDDFT) provides access to the excited states. We have implemented the two common formulations of TDDFT, namely the linear-response and the time propagation schemes. Electron transport calculations under finite-bias conditions can be performed with GPAW using non-equilibrium Green functions and the localized basis set. In addition to the basic features of the real-space PAW method, we also describe the implementation of selected exchange-correlation functionals, parallelization schemes, ΔSCF-method, x-ray absorption spectra, and maximally localized Wannier orbitals.
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