Second-Order Moller-Plesset Perturbation (MP2) Theory at Finite Temperature: Relation with Surjan's Density Matrix MP2 and Its Application to Linear-Scaling Divide-and-Conquer Method
Second-Order Moller-Plesset Perturbation (MP2) Theory at Finite Temperature: Relation with Surjan's Density Matrix MP2 and Its Application to Linear-Scaling Divide-and-Conquer Method
复制标题
有限温度下的二阶 Moller-Plesset 微扰 (MP2) 理论:与 Surjan 密度矩阵 MP2 的关系及其在线性标度分治法中的应用
DOI:
10.1007/s00214-015-1710-y
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发表时间:
2015
期刊:
影响因子:
--
通讯作者:
T. Taketsugu
中科院分区:
文献类型:
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作者:
M. Kobayashi;T. Taketsugu
In 2005, Surján showed two explicit formulas for evaluating the second-order Møller–Plesset perturbation (MP2) energy as a functional of the Hartree–Fock density matrix $$\varvec{D}$$ (Chem Phys Lett 406:318, 2005), which are referred to as the $$\Delta E_\text {MP2}[\varvec{D}]$$ functionals. In this paper, we present the finite-temperature (FT) MP2 energy functionals of the FT Hartree–Fock density matrix. There are also two formulas for the FT-MP2, namely the conventional and renormalized ones; the latter of which has recently been formulated by Hirata and He (J Chem Phys 138:204112, 2013). We proved that there exists one-to-one correspondence between the formulas of two FT-MP2 and the $$\Delta E_\text {MP2}[\varvec{D}]$$ functionals. This fact can explain the different behavior of two $$\Delta E_\text {MP2}[\varvec{D}]$$ functionals when an approximate Hartree–Fock density matrix is applied, which was previously investigated by Kobayashi and Nakai (Chem Phys Lett 420:250, 2006). We also applied the FT-MP2 formalisms to the linear-scaling divide-and-conquer method for improving the accuracy with tiny addition of the computational efforts.