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arXiv 1804.01037physics.chem-phcond-mat.mtrl-sci
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从近似运动方程环耦合团簇双态计算无规相近似激发能

Random-phase approximation excitation energies from approximate equation-of-motion ring coupled-cluster doubles

Timothy C. Berkelbach

摘要:

在随机相位近似(RPA)中计算的基态相关能是已知的是相同的,使用一个子集的条款出现在耦合团簇理论与双激发计算。特别是,这种等价性要求只保留那些在戈德斯通意义上产生与时间无关的环图的项。在这里,我表明,这种等价性延伸到中性激发能,在RPA中计算的是相同的那些使用近似运动方程耦合团簇理论与双激发(EOM-CCD)。这种等效性需要对EOM-CCD进行三种近似:首先,从环形CCD方程出发,得到基态双激发振幅(与相关能相同);其次,将EOM本征值问题截断为单激励问题(单粒子+单空穴)子空间;第三,必须忽略Fock算子的相似变换,因为它对应于单粒子传播子的修饰,这在传统RPA中是不存在的。

英文摘要:

The ground-state correlation energy calculated in the random-phase approximation (RPA) is known to be identical to that calculated using a subset of terms appearing in coupled-cluster theory with double excitations. In particular, this equivalence requires keeping only those terms that generate time-independent ring diagrams, in the Goldstone sense. Here I show that this equivalence extends to neutral excitation energies, for which those calculated in the RPA are identical to those calculated using an approximation to equation-of-motion coupled-cluster theory with double excitations (EOM-CCD). The equivalence requires three approximations to EOM-CCD: first, the ground-state double-excitation amplitudes are obtained from the ring-CCD equations (the same as for the correlation energy); second, the EOM eigenvalue problem is truncated to the single-excitation (one particle + one hole) subspace; third, the similarity transformation of the Fock operator must be neglected, as it corresponds to a dressing of the single-particle propagator, which is not present in the conventional RPA.

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