arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2011.11601physics.chem-ph
收藏

用于势能面的Δ-机器学习:一种将基于DFT的PES提升至CCSD(T)理论水平的PIP方法

$Δ$-Machine Learning for Potential Energy Surfaces: A PIP approach to bring a DFT-based PES to CCSD(T) Level of Theory

Emory University(埃默里大学);University of Maryland, College Park(马里兰大学帕克分校);Cornell University(康奈尔大学);Georgia Institute of Technology(佐治亚理工学院);Università Degli Studi di Milano(米兰大学)

Apurba Nandi, Chen Qu, Paul Houston, Riccardo Conte, Joel M. Bowman

AI总结:

本研究提出基于置换不变多项式(PIP)的Δ-机器学习方法,通过低阶PIP基组拟合少量CCSD(T)能量校正DFT级PES,仅用数百至数千个CCSD(T)能量即可将多分子势能面提升至接近CCSD(T)精度。

摘要:

“Δ-机器学习”是指一种将基于低水平(LL)密度泛函理论(DFT)能量与梯度的势能面(PES)等属性提升至接近耦合簇(CC)精度水平的机器学习方法。本文提出了一种采用置换不变多项式(PIP)方法拟合高维PES的此类方法。该方法可由一个简单方程表示,符号含义清晰:$V_{LL{\rightarrow}CC}=V_{LL}+Δ{V_{CC-LL}}$,并在甲烷($\boldsymbol{\text{CH}_4}$)、水合氢离子($\boldsymbol{\text{H}_3\text{O}^+}$)以及反式和顺式-N-甲基乙酰胺(NMA,$\boldsymbol{\text{CH}_3\text{CONHCH}_3}$)体系上进行了验证。对于这些分子,低水平PES即$V_{LL}$是对DFT/B3LYP/6-31+G(d)能量和梯度的PIP拟合,而$Δ{V_{CC-LL}}$则是采用低阶PIP基组、基于相对少量CCSD(T)能量得到的精确PIP拟合。其中,针对$\text{CH}_4$采用了aug-cc-pVDZ基组的新计算结果,针对$\text{H}_3\text{O}^+$使用了已有的CCSD(T)-F12/aug-cc-pVQZ能量数据,针对NMA则开展了新的CCSD(T)-F12/aug-cc-pVDZ计算。仅需少至200个CCSD(T)能量,新得到的PES就与小分子的基准CCSD(T)结果高度吻合;对于含12个原子的NMA,使用4696个CCSD(T)能量完成了训练。

英文摘要:

``$Δ$-machine learning" refers to a machine learning approach to bring a property such as a potential energy surface (PES) based on low-level (LL) density functional theory (DFT) energies and gradients to close to a coupled cluster (CC) level of accuracy. Here we present such an approach that uses the permutationally invariant polynomial (PIP) method to fit high-dimensional PESs. The approach is represented by a simple equation, in obvious notation $V_{LL{\rightarrow}CC}=V_{LL}+Δ{V_{CC-LL}}$, and demonstrated for \ce{CH4}, \ce{H3O+}, and $trans$ and $cis$-$N$-methyl acetamide (NMA), \ce{CH3CONHCH3}. For these molecules, the LL PES, $V_{LL}$, is a PIP fit to DFT/B3LYP/6-31+G(d) energies and gradients, and $Δ{V_{CC-LL}}$ is a precise PIP fit obtained using a low-order PIP basis set and based on a relatively small number of CCSD(T) energies. For \ce{CH4} these are new calculations adopting an aug-cc-pVDZ basis, for \ce{H3O+} previous CCSD(T)-F12/aug-cc-pVQZ energies are used, while for NMA new CCSD(T)-F12/aug-cc-pVDZ calculations are performed. With as few as 200 CCSD(T) energies, the new PESs are in excellent agreement with benchmark CCSD(T) results for the small molecules, and for 12-atom NMA training is done with 4696 CCSD(T) energies.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑