In Green's function theory, the total energy of an interacting many-electronsystem can be expressed in a variational form using the Klein or Luttinger-Wardfunctionals. Green's function theory also naturally addresses the case wherethe interacting system is embedded into a bath. This latter can then act as adynamical (i.e., frequency-dependent) potential, providing a more generalframework than that of conventional static external potentials. Notably, theKlein functional includes a term of the form $\text{Tr}_\omega\text{Ln}\left\{G_0^{-1}G\right\}$, where $\text{Tr}_\omega$ is the frequencyintegration of the trace operator. Here, we show that using a sum-over-polerepresentation for the Green's functions and the algorithmic-inversion methodone can obtain in full generality an explicit analytical expression for$\text{Tr}_\omega \text{Ln}\left\{G_0^{-1}G\right\}$. This allows one, e.g., toderive a variational expression for the Klein functional in the presence of anembedding bath, or to provide an explicit expression of the RPA correlationenergy in the framework of the optimized effective potential.

Green's function embedding using sum-over-pole representations

Andrea Ferretti
;
2024

Abstract

In Green's function theory, the total energy of an interacting many-electronsystem can be expressed in a variational form using the Klein or Luttinger-Wardfunctionals. Green's function theory also naturally addresses the case wherethe interacting system is embedded into a bath. This latter can then act as adynamical (i.e., frequency-dependent) potential, providing a more generalframework than that of conventional static external potentials. Notably, theKlein functional includes a term of the form $\text{Tr}_\omega\text{Ln}\left\{G_0^{-1}G\right\}$, where $\text{Tr}_\omega$ is the frequencyintegration of the trace operator. Here, we show that using a sum-over-polerepresentation for the Green's functions and the algorithmic-inversion methodone can obtain in full generality an explicit analytical expression for$\text{Tr}_\omega \text{Ln}\left\{G_0^{-1}G\right\}$. This allows one, e.g., toderive a variational expression for the Klein functional in the presence of anembedding bath, or to provide an explicit expression of the RPA correlationenergy in the framework of the optimized effective potential.
2024
Istituto Nanoscienze - NANO
Istituto Nanoscienze - NANO - Sede Secondaria Modena
Physics - Materials Science
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/473682
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