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Embedding theory for excited states

机译:激发态的嵌入理论

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Using the technique of Perdew and Levy [Phys. Rev. B 31, 6264 (1985)], it is shown that both the density function theory (DFT)-in-DFT and wave function theory (WFT)-in-DFT embedding approaches are formally correct in studying not only the ground state but also a subset of the excited states of the total system. Without further approximations, the DFT-in-DFT embedding approach results in a pair of coupled Euler-Lagrange equations. In contrast to DFT-in-DFT, the WFT-in-DFT approach is shown to ensure a systematic description of excited states if such states are mainly related to excitations within the embedded subsystem. Possible ways for the practical realization of the WFT-in-DFT approach for studying excited states are briefly discussed.
机译:使用Perdew和Levy的技术[Phys。 Rev. B 31,6264(1985)]表明,DFT中的密度函数理论(DFT)和DFT中的波函数理论(WFT)嵌入方法在研究基态方面不仅形式正确,也是整个系统激发态的子集。在没有进一步近似的情况下,DFT-in-DFT嵌入方法可生成一对耦合的Euler-Lagrange方程。与DFT-in-DFT相比,WFT-in-DFT方法可确保对激发态进行系统描述,如果这些状态主要与嵌入式子系统内的激发有关。简要讨论了用于研究激发态的WFT-in-DFT方法的实际实现方式。

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