one more Paola ref
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\begin{thebibliography}{178}%
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10.1063/1.5078565} {\bibfield {journal} {\bibinfo {journal} {J. Chem.
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10.1063/1.5078565} {\bibfield {journal} {\bibinfo {journal} {J. Chem.
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Phys.}\ }\textbf {\bibinfo {volume} {149}},\ \bibinfo {pages} {241101}
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Phys.}\ }\textbf {\bibinfo {volume} {149}},\ \bibinfo {pages} {241101}
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(\bibinfo {year} {2018})}\BibitemShut {NoStop}%
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(\bibinfo {year} {2018})}\BibitemShut {NoStop}%
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\bibitem [{\citenamefont {Daas}\ \emph {et~al.}(2020)\citenamefont {Daas},
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\citenamefont {Grossi}, \citenamefont {Vuckovic}, \citenamefont {Musslimani},
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\citenamefont {Kooi}, \citenamefont {Seidl}, \citenamefont {Giesbertz},\ and\
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\citenamefont {Gori-Giorgi}}]{Daas_2020}%
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\bibfield {author} {\bibinfo {author} {\bibfnamefont {T.~J.}\ \bibnamefont
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{Daas}}, \bibinfo {author} {\bibfnamefont {J.}~\bibnamefont {Grossi}},
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\bibinfo {author} {\bibfnamefont {S.}~\bibnamefont {Vuckovic}}, \bibinfo
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{author} {\bibfnamefont {Z.~H.}\ \bibnamefont {Musslimani}}, \bibinfo
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{author} {\bibfnamefont {D.~P.}\ \bibnamefont {Kooi}}, \bibinfo {author}
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{\bibfnamefont {M.}~\bibnamefont {Seidl}}, \bibinfo {author} {\bibfnamefont
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{K.~J.~H.}\ \bibnamefont {Giesbertz}}, \ and\ \bibinfo {author}
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{\bibfnamefont {P.}~\bibnamefont {Gori-Giorgi}},\ }\href {\doibase
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10.1063/5.0029084} {\bibfield {journal} {\bibinfo {journal} {J. Chem.
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Phys.}\ }\textbf {\bibinfo {volume} {153}},\ \bibinfo {pages} {214112}
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\bibitem [{\citenamefont {Bartlett}\ and\ \citenamefont
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\bibitem [{\citenamefont {Bartlett}\ and\ \citenamefont
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{Silver}(1975)}]{Bartlett_1975}%
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{Silver}(1975)}]{Bartlett_1975}%
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%% This BibTeX bibliography file was created using BibDesk.
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%% This BibTeX bibliography file was created using BibDesk.
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%% Created for Pierre-Francois Loos at 2020-12-05 15:45:56 +0100
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%% Created for Pierre-Francois Loos at 2020-12-05 22:01:16 +0100
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@article{Daas_2020,
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author = {Daas,Timothy J. and Grossi,Juri and Vuckovic,Stefan and Musslimani,Ziad H. and Kooi,Derk P. and Seidl,Michael and Giesbertz,Klaas J. H. and Gori-Giorgi,Paola},
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date-added = {2020-12-05 21:58:26 +0100},
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date-modified = {2020-12-05 22:01:16 +0100},
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doi = {10.1063/5.0029084},
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journal = {J. Chem. Phys.},
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number = {21},
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pages = {214112},
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title = {Large coupling-strength expansion of the M{\o}ller--Plesset adiabatic connection: From paradigmatic cases to variational expressions for the leading terms},
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volume = {153},
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year = {2020},
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Bdsk-Url-1 = {https://doi.org/10.1063/5.0029084}}
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@article{Barca_2014,
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@article{Barca_2014,
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author = {G. M. J. Barca and A. T. B. Gilbert and P. M. W. Gill},
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author = {G. M. J. Barca and A. T. B. Gilbert and P. M. W. Gill},
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date-added = {2020-12-05 15:45:52 +0100},
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date-added = {2020-12-05 15:45:52 +0100},
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@ -732,7 +733,7 @@ Although practically convenient for electronic structure calculations, the MP pa
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the only possibility and alternative partitionings have been considered including:
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the only possibility and alternative partitionings have been considered including:
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i) the Epstein-Nesbet (EN) partitioning which consists in taking the diagonal elements of $\hH$ as the zeroth-order Hamiltonian, \cite{Nesbet_1955,Epstein_1926}
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i) the Epstein-Nesbet (EN) partitioning which consists in taking the diagonal elements of $\hH$ as the zeroth-order Hamiltonian, \cite{Nesbet_1955,Epstein_1926}
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ii) the weak correlation partitioning in which the one-electron part is consider as the unperturbed Hamiltonian $\hH^{(0)}$ and the two-electron part is the perturbation operator $\hV$, and
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ii) the weak correlation partitioning in which the one-electron part is consider as the unperturbed Hamiltonian $\hH^{(0)}$ and the two-electron part is the perturbation operator $\hV$, and
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iii) the strong coupling partitioning where the two operators are inverted compared to the weak correlation partitioning. \cite{Seidl_2018}
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iii) the strong coupling partitioning where the two operators are inverted compared to the weak correlation partitioning. \cite{Seidl_2018,Daas_2020}
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While an in-depth comparison of these different approaches can offer insight into
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While an in-depth comparison of these different approaches can offer insight into
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their relative strengths and weaknesses for various situations, we will restrict our current discussion
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their relative strengths and weaknesses for various situations, we will restrict our current discussion
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to the convergence properties of the MP expansion.
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to the convergence properties of the MP expansion.
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