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Pierre-Francois Loos 2021-01-19 17:10:41 +01:00
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Manuscript/sfBSE.bib
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@ -1,13 +1,26 @@
%% This BibTeX bibliography file was created using BibDesk. %% This BibTeX bibliography file was created using BibDesk.
%% http://bibdesk.sourceforge.net/ %% http://bibdesk.sourceforge.net/
%% Created for Pierre-Francois Loos at 2021-01-19 16:50:28 +0100 %% Created for Pierre-Francois Loos at 2021-01-19 17:10:17 +0100
%% Saved with string encoding Unicode (UTF-8) %% Saved with string encoding Unicode (UTF-8)
@article{Li_2021,
author = {Li, Jing and Olevano, Valerio},
date-added = {2021-01-19 17:08:27 +0100},
date-modified = {2021-01-19 17:10:13 +0100},
doi = {10.1103/PhysRevA.103.012809},
journal = {Phys. Rev. A},
pages = {012809},
title = {Hydrogen-molecule spectrum by the many-body $GW$ approximation and the Bethe-Salpeter equation},
volume = {103},
year = {2021},
Bdsk-Url-1 = {https://link.aps.org/doi/10.1103/PhysRevA.103.012809},
Bdsk-Url-2 = {https://doi.org/10.1103/PhysRevA.103.012809}}
@article{Vitale_2020, @article{Vitale_2020,
author = {Vitale, Eugenio and Alavi, Ali and Kats, Daniel}, author = {Vitale, Eugenio and Alavi, Ali and Kats, Daniel},
date-added = {2021-01-17 22:10:20 +0100}, date-added = {2021-01-17 22:10:20 +0100},

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Manuscript/sfBSE.tex
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@ -850,7 +850,7 @@ Finally, both SF-ADC(2)-x and SF-ADC(3) yield excitation energies very close to
\label{sec:H2} \label{sec:H2}
%=============================== %===============================
Our second example deals with the dissociation of the \ce{H2} molecule, which is a prototypical system for testing new electronic structure methods and, specifically, their accuracy in the presence of strong correlation (see, for example, Refs.~\onlinecite{Caruso_2013,Barca_2014,Vuckovic_2017}, and references therein). Our second example deals with the dissociation of the \ce{H2} molecule, which is a prototypical system for testing new electronic structure methods and, specifically, their accuracy in the presence of strong correlation (see, for example, Refs.~\onlinecite{Caruso_2013,Barca_2014,Vuckovic_2017,Li_2021}, and references therein).
The $\text{X}\,{}^1 \Sigma_g^+$ ground state of \ce{H2} has an electronic configuration $(1\sigma_g)^2$ configuration. The $\text{X}\,{}^1 \Sigma_g^+$ ground state of \ce{H2} has an electronic configuration $(1\sigma_g)^2$ configuration.
The variation of the excitation energies associated with the three lowest singlet excited states with respect to the elongation of the \ce{H-H} bond are of particular interest here. The variation of the excitation energies associated with the three lowest singlet excited states with respect to the elongation of the \ce{H-H} bond are of particular interest here.
The lowest singly excited state $\text{B}\,{}^1 \Sigma_u^+$ has a $(1\sigma_g )(1\sigma_u)$ configuration, while the singly excited state $\text{E}\,{}^1 \Sigma_g^+$ and the doubly excited state $\text{F}\,{}^1 \Sigma_g^+$ have $(1\sigma_g ) (2\sigma_g)$ and $(1\sigma_u )(1\sigma_u)$ configurations, respectively. The lowest singly excited state $\text{B}\,{}^1 \Sigma_u^+$ has a $(1\sigma_g )(1\sigma_u)$ configuration, while the singly excited state $\text{E}\,{}^1 \Sigma_g^+$ and the doubly excited state $\text{F}\,{}^1 \Sigma_g^+$ have $(1\sigma_g ) (2\sigma_g)$ and $(1\sigma_u )(1\sigma_u)$ configurations, respectively.