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激发态平均场理论的自洽场公式

A self-consistent field formulation of excited state mean field theory.

作者信息

Hardikar Tarini S, Neuscamman Eric

机构信息

Department of Chemistry, University of California, Berkeley, California 94720, USA.

出版信息

J Chem Phys. 2020 Oct 28;153(16):164108. doi: 10.1063/5.0019557.

Abstract

We show that, as in Hartree-Fock theory, the orbitals for excited state mean field theory can be optimized via a self-consistent one-electron equation in which electron-electron repulsion is accounted for through mean field operators. In addition to showing that this excited state ansatz is sufficiently close to a mean field product state to admit a one-electron formulation, this approach brings the orbital optimization speed to within roughly a factor of two of ground state mean field theory. The approach parallels Hartree Fock theory in multiple ways, including the presence of a commutator condition, a one-electron mean-field working equation, and acceleration via direct inversion in the iterative subspace. When combined with a configuration interaction singles Davidson solver for the excitation coefficients, the self-consistent field formulation dramatically reduces the cost of the theory compared to previous approaches based on quasi-Newton descent.

摘要

我们表明,与哈特里 - 福克理论一样,激发态平均场理论的轨道可以通过自洽单电子方程进行优化,其中电子 - 电子排斥通过平均场算符来考虑。除了表明这种激发态假设足够接近平均场乘积态以允许单电子表述外,这种方法还将轨道优化速度提高到了基态平均场理论的大约两倍以内。该方法在多个方面与哈特里 - 福克理论相似,包括存在对易子条件、单电子平均场工作方程以及通过迭代子空间中的直接反演进行加速。当与用于激发系数的组态相互作用单重态戴维森求解器相结合时,与基于拟牛顿下降的先前方法相比,自洽场表述显著降低了该理论的成本。

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