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多参考扩散蒙特卡罗方法应用于二维材料。

Multireference diffusion Monte Carlo reaches 2D materials.

作者信息

Spanedda Nicole, Benali Anouar, Reboredo Fernando A, Krogel Jaron T

机构信息

Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, USA.

Computational Science Division, Argonne National Laboratory, Lemont, USA.

出版信息

Sci Rep. 2025 Sep 26;15(1):32984. doi: 10.1038/s41598-025-17564-3.

DOI:10.1038/s41598-025-17564-3
PMID:41006441
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC12475236/
Abstract

Quantum confinement in 2D materials strongly enhances electronic correlation effects. Therefore, predicting the properties of these unique materials, with both a high level of accuracy and computational efficiency, without relying on adjustable parameters or functionals, remains an outstanding theoretical challenge. The majority of theoretical studies are based on the approximations of density functional theory (DFT). The reliability of DFT predictions are heavily dependent on the choice of an approximated exchange-correlation functional. Here, we estimate the magnitude of impact of correlation on the total energy for the quintessential 2D material, graphene, by performing and comparing state-of-the-art selected CI and quantum Monte Carlo extrapolated calculations for a single unit cell at the Γ point. We demonstrate that Self-Healing Diffusion Monte Carlo (SHDMC) obtains a very compact, but high-quality wavefunction for this system that lacks the strong basis set dependence displayed by state of the art quantum chemistry methods. The SHDMC wavefunction is of higher quality compared to that obtained from sCI, in the same orbital basis, while being ∼ 1000 times smaller in terms of determinant count compared to sCI. We also demonstrate that extrapolating SHDMC results to the infinite determinant limit compares extremely well with complete basis set extrapolated sCI. Our work paves the way for future validation of SHDMC applied to challenging 2D materials.

摘要

二维材料中的量子限域强烈增强了电子关联效应。因此,在不依赖可调参数或泛函的情况下,以高精度和计算效率预测这些独特材料的性质仍然是一个突出的理论挑战。大多数理论研究基于密度泛函理论(DFT)的近似。DFT预测的可靠性在很大程度上取决于近似交换关联泛函的选择。在这里,我们通过在Γ点对单个晶胞进行并比较最先进的选定CI和量子蒙特卡罗外推计算,来估计关联对典型二维材料石墨烯总能量的影响程度。我们证明,自愈合扩散蒙特卡罗(SHDMC)为该系统获得了一个非常紧凑但高质量的波函数,该波函数没有最先进量子化学方法所显示的对基组的强烈依赖性。与在相同轨道基组下从sCI获得的波函数相比,SHDMC波函数质量更高,而在行列式数量方面比sCI小约1000倍。我们还证明,将SHDMC结果外推到无限行列式极限与完全基组外推的sCI相比非常吻合。我们的工作为未来将SHDMC应用于具有挑战性的二维材料的验证铺平了道路。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/b1908db1a822/41598_2025_17564_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/c10f92e38f0d/41598_2025_17564_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/b9deb93c7000/41598_2025_17564_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/2a8b4a7747ba/41598_2025_17564_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/978fc4df8f06/41598_2025_17564_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/0d96722d77c1/41598_2025_17564_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/74509e3ea1ec/41598_2025_17564_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/b1908db1a822/41598_2025_17564_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/c10f92e38f0d/41598_2025_17564_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/b9deb93c7000/41598_2025_17564_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/2a8b4a7747ba/41598_2025_17564_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/978fc4df8f06/41598_2025_17564_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/0d96722d77c1/41598_2025_17564_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/74509e3ea1ec/41598_2025_17564_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5636/12475236/b1908db1a822/41598_2025_17564_Fig7_HTML.jpg

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Diffusion Monte Carlo method on small boron clusters using single- and multi- determinant-Jastrow trial wavefunctions.
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