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用于排斥哈密顿量的自旋多项式相似变换:在耦合簇和自旋投影无限制哈特里 - 福克之间进行插值

Spin polynomial similarity transformation for repulsive Hamiltonians: interpolating between coupled cluster and spin-projected unrestricted Hartree-Fock.

作者信息

Gomez John A, Degroote Matthias, Zhao Jinmo, Qiu Yiheng, Scuseria Gustavo E

机构信息

Department of Chemistry, Rice University, Houston, TX 77005, USA.

出版信息

Phys Chem Chem Phys. 2017 Aug 23;19(33):22385-22394. doi: 10.1039/c7cp04075j.

Abstract

Our overarching goal is to be able to describe both weak and strong correlation with a single, computationally affordable method without sacrificing important qualities of the wavefunction, e.g. symmetries of the Hamiltonian. We know that coupled cluster theory with low-order excitations is excellent at describing weakly-correlated systems near equilibrium, but breaks down as systems become more strongly correlated. Projected Hartree-Fock on the other hand is inherently capable of describing multireference character, but misses weak correlation. We are thus exploring how best to combine coupled cluster and projected Hartree-Fock in our search for a computationally feasible method that is applicable across a wide range of correlation strengths. In this manuscript, we adapt our earlier work on the pairing Hamiltonian to repulsive Hamiltonians, resulting in the spin polynomial similarity transformation (SpinPoST) interpolation. SpinPoST parameterizes the wavefunction in order to interpolate between the coupled cluster and spin-projected unrestricted Hartree-Fock ansätze self consistently, and is a spin-symmetry adapted model which involves only single and double excitations. We employ a unique approach of optimizing the wavefunction by minimizing the effect of connected quadruple excitations, resulting in a method which is spin-symmetry adapted and is comparable energetically to coupled cluster with singles and doubles for weak correlation and spin-projected Hartree-Fock for strong correlation.

摘要

我们的总体目标是,能够用一种计算成本可承受的单一方法来描述弱关联和强关联,同时又不牺牲波函数的重要性质,例如哈密顿量的对称性。我们知道,具有低阶激发的耦合簇理论在描述接近平衡的弱关联系统方面表现出色,但随着系统关联度增强会失效。另一方面,投影哈特里 - 福克理论本质上能够描述多参考特征,但会忽略弱关联。因此,我们正在探索如何最佳地结合耦合簇理论和投影哈特里 - 福克理论,以寻找一种计算上可行的方法,该方法适用于广泛的关联强度范围。在本论文中,我们将之前关于配对哈密顿量的工作应用于排斥性哈密顿量,从而得到自旋多项式相似变换(SpinPoST)插值法。SpinPoST对波函数进行参数化,以便在耦合簇和自旋投影无限制哈特里 - 福克近似之间自洽地进行插值,并且是一种仅涉及单激发和双激发的自旋对称适配模型。我们采用了一种独特的方法,即通过最小化连通四重激发的影响来优化波函数,从而得到一种自旋对称适配的方法,对于弱关联,其能量与单双激发耦合簇相当,对于强关联,其能量与自旋投影哈特里 - 福克相当。

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