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Coupled-cluster theories for the polarizable continuum model. II. analytical gradients for excited states of molecular solutes by the equation of motion coupled-cluster method

机译:可极化连续体模型的耦​​合簇理论。二。运动耦合簇法求解分子溶质激发态的解析梯度

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The theory for the analytical energy gradients of excited electronic state described by equation of motion couped-cluster method (EOM-CC) (Stanton, J Chem Phys, 1993, 99, 8840) has been generalized to molecules in solution within the polarizable continuum model (PCM) framework (Miertu? et al. Chem Phys 1981, 55, 117). The final equations of the PCM-EOM gradients are developed at the single and double excitation level (CCSD) and are cast in a form similar to that developed for the ground state CC energy derivatives of solvated molecules (Cammi, J Chem Phys 2009, 131, 164104), involving contraction of effective one- and two-particle density matrices with differentiated one- and two-electron integrals over atomic orbitals.
机译:通过运动偶合簇方法方程(EOM-CC)(Stanton,J Chem Phys,1993,99,8840)描述的用于激发电子态的分析能梯度的理论已经推广到可极化连续体模型中的溶液中的分子(PCM)框架(Miertu?et al。Chem Phys 1981,55,117)。 PCM-EOM梯度的最终方程式是在单激发和双激发能级(CCSD)上开发的,其形式类似于为溶剂化分子的基态CC能量衍生物开发的形式(Cammi,J Chem Phys 2009,131 ,164164),涉及有效的一粒子密度和二粒子密度矩阵的收缩,以及在原子轨道上具有差分的一电子和二电子积分。

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