Generalizing deep learning electronic structure calculation to the plane-wave basis.

IF 12 Q1 COMPUTER SCIENCE, INTERDISCIPLINARY APPLICATIONS
Xiaoxun Gong, Steven G Louie, Wenhui Duan, Yong Xu
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引用次数: 0

Abstract

Deep neural networks capable of representing the density functional theory (DFT) Hamiltonian as a function of material structure hold great promise for revolutionizing future electronic structure calculations. However, a notable limitation of previous neural networks is their compatibility solely with the atomic-orbital (AO) basis, excluding the widely used plane-wave (PW) basis. Here we overcome this critical limitation by proposing an accurate and efficient real-space reconstruction method for directly computing AO Hamiltonian matrices from PW DFT results. The reconstruction method is orders of magnitude faster than traditional projection-based methods to convert PW results to the AO basis, and the reconstructed Hamiltonian matrices can faithfully reproduce the PW electronic structure, thus bridging the longstanding gap between the AO basis deep learning electronic structure approach and PW DFT. Advantages of the PW methods, such as high accuracy, high flexibility and wide applicability, thus can be all integrated into deep learning electronic structure methods without sacrificing these methods' inherent benefits. This allows for the construction of large-scale and high-fidelity training datasets with the help of PW DFT results towards the development of precise and broadly applicable deep learning electronic structure models.

将深度学习电子结构计算推广到平面波基础。
能够将密度泛函理论(DFT)哈密顿表示为材料结构函数的深度神经网络,为未来电子结构计算的变革带来了巨大希望。然而,以往神经网络的一个显著局限是只兼容原子轨道(AO)基础,而不兼容广泛使用的平面波(PW)基础。在此,我们提出了一种精确而高效的实空间重构方法,用于从 PW DFT 结果中直接计算 AO 哈密顿矩阵,从而克服了这一关键限制。与传统的基于投影的方法相比,这种重构方法将 PW 结果转换为 AO 基的速度快了几个数量级,而且重构的哈密顿矩阵可以忠实地再现 PW 电子结构,从而弥补了 AO 基深度学习电子结构方法与 PW DFT 之间长期存在的差距。因此,PW 方法的优势,如高精度、高灵活性和广泛适用性,可以在不牺牲这些方法固有优势的前提下,全部集成到深度学习电子结构方法中。这样,在 PW DFT 结果的帮助下,就可以构建大规模、高保真的训练数据集,从而开发出精确、广泛适用的深度学习电子结构模型。
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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来源期刊
CiteScore
11.70
自引率
0.00%
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