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消除有限温度电子结构计算中的基组不完备误差:双电子体系

Removing Basis Set Incompleteness Error in Finite-Temperature Electronic Structure Calculations: Two-Electron Systems.

作者信息

Van Benschoten William Z, Shepherd James J

机构信息

Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, United States.

出版信息

J Phys Chem A. 2024 Dec 12;128(49):10659-10672. doi: 10.1021/acs.jpca.4c03769. Epub 2024 Nov 25.

DOI:10.1021/acs.jpca.4c03769
PMID:39585915
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11647908/
Abstract

We investigate the basis-set-size dependence for quantities related to interacting electrons in the canonical ensemble. Calculations are performed using exact diagonalization (finite temperature full configuration interaction method) on two-electron model systems─the uniform electron gas (UEG) and the helium atom. Our data reproduce previous observations of a competition for how the internal energy converges between the ground-state correlation energy and the high-temperature kinetic energy. We explore how this can be related to component parts of the internal energy including kinetic, exchange, and correlation energies and show there is surprising nuance in how this can be broken down into mostly monotonically converging quantities. We also show that separation of the free energy into a free energy with/without correlation allows for monotonic convergence with basis set size due to the variational principle. We find that the free energy convergence matches the previously observed convergence properties of the internal energy. We discuss the free energy divergence that happens when converging a finite basis analytical hydrogen atom to the complete basis set limit and compare this to the energies of a helium atom in a large periodic box. Reducing the box size, we saw convergence trends for the helium atom that were similar to the UEG.

摘要

我们研究了正则系综中与相互作用电子相关的量对基组大小的依赖性。使用精确对角化(有限温度全组态相互作用方法)对双电子模型系统——均匀电子气(UEG)和氦原子进行了计算。我们的数据重现了先前关于基态关联能和高温动能之间内能如何收敛的竞争的观察结果。我们探讨了这如何与内能的组成部分(包括动能、交换能和关联能)相关,并表明在如何将其分解为大多单调收敛的量方面存在惊人的细微差别。我们还表明,由于变分原理,将自由能分离为有/无关联的自由能允许与基组大小单调收敛。我们发现自由能收敛与先前观察到的内能收敛特性相匹配。我们讨论了将有限基分析氢原子收敛到完整基组极限时发生的自由能发散,并将其与大周期盒中氦原子的能量进行比较。减小盒尺寸时,我们看到氦原子的收敛趋势与均匀电子气相似。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/94a955caa2f9/jp4c03769_0010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/cea7f59ef7c7/jp4c03769_0001.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/81b2ca46a810/jp4c03769_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/d5d997bae106/jp4c03769_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/24cbc6ea4270/jp4c03769_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/70108931a0a4/jp4c03769_0007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/fc140b640e3f/jp4c03769_0008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/70946f437bf4/jp4c03769_0009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/94a955caa2f9/jp4c03769_0010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/cea7f59ef7c7/jp4c03769_0001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/fef66c91f0d8/jp4c03769_0002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/0fd268c30552/jp4c03769_0003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/81b2ca46a810/jp4c03769_0004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/d5d997bae106/jp4c03769_0005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/24cbc6ea4270/jp4c03769_0006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/70108931a0a4/jp4c03769_0007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/fc140b640e3f/jp4c03769_0008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/70946f437bf4/jp4c03769_0009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/9aea/11647908/94a955caa2f9/jp4c03769_0010.jpg

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本文引用的文献

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Toward Real Chemical Accuracy on Current Quantum Hardware Through the Transcorrelated Method.通过转相关方法在当前量子硬件上实现真正的化学精度。
J Chem Theory Comput. 2024 May 28;20(10):4146-4160. doi: 10.1021/acs.jctc.4c00070. Epub 2024 May 9.
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J Chem Phys. 2023 Oct 28;159(16). doi: 10.1063/5.0171930.
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