intro
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%Control: page (0) single
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\begin{thebibliography}{153}%
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\begin{thebibliography}{154}%
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\makeatletter
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\providecommand \@ifxundefined [1]{%
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\@ifx{#1\undefined}
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{Plesset}},\ }\href {\doibase 10.1103/PhysRev.46.618} {\bibfield {journal}
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{\bibinfo {journal} {Phys. Rev.}\ }\textbf {\bibinfo {volume} {46}},\
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\bibinfo {pages} {618} (\bibinfo {year} {1934})}\BibitemShut {NoStop}%
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\bibitem [{\citenamefont {Wigner}(1934)}]{Wigner_1934}%
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\BibitemOpen
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\bibfield {author} {\bibinfo {author} {\bibfnamefont {E.}~\bibnamefont
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{Wigner}},\ }\href {\doibase 10.1103/PhysRev.46.1002} {\bibfield {journal}
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{\bibinfo {journal} {Phys. Rev.}\ }\textbf {\bibinfo {volume} {46}},\
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\bibinfo {pages} {1002} (\bibinfo {year} {1934})}\BibitemShut {NoStop}%
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\bibitem [{\citenamefont {L\"owdin}(1958)}]{Lowdin_1958}%
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\BibitemOpen
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\bibfield {author} {\bibinfo {author} {\bibfnamefont {P.-O.}\ \bibnamefont
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{L\"owdin}},\ }\enquote {\bibinfo {title} {Correlation problem in
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many-electron quantum mechanics i. review of different approaches and
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discussion of some current ideas},}\ in\ \href {\doibase
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https://doi.org/10.1002/9780470143483.ch7} {\emph {\bibinfo {booktitle} {Adv.
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Chem. Phys.}}}\ (\bibinfo {publisher} {John Wiley \& Sons, Ltd},\ \bibinfo
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{year} {1958})\ pp.\ \bibinfo {pages} {207--322}\BibitemShut {NoStop}%
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\bibitem [{\citenamefont {Laidig}\ \emph {et~al.}(1985)\citenamefont {Laidig},
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\citenamefont {Fitzgerald},\ and\ \citenamefont {Bartlett}}]{Laidig_1985}%
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\BibitemOpen
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10.1140/epjb/e2018-90114-9} {\bibfield {journal} {\bibinfo {journal} {Eur.
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Phys. J. B}\ }\textbf {\bibinfo {volume} {91}},\ \bibinfo {pages} {142}
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(\bibinfo {year} {2018})}\BibitemShut {NoStop}%
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\bibitem [{\citenamefont {Wigner}(1934)}]{Wigner_1934}%
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\BibitemOpen
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\bibfield {author} {\bibinfo {author} {\bibfnamefont {E.}~\bibnamefont
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{Wigner}},\ }\href {\doibase 10.1103/PhysRev.46.1002} {\bibfield {journal}
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{\bibinfo {journal} {Phys. Rev.}\ }\textbf {\bibinfo {volume} {46}},\
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\bibinfo {pages} {1002} (\bibinfo {year} {1934})}\BibitemShut {NoStop}%
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\bibitem [{\citenamefont {Cejnar}\ \emph {et~al.}(2007)\citenamefont {Cejnar},
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\citenamefont {Heinze},\ and\ \citenamefont {Macek}}]{Cejnar_2007}%
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\BibitemOpen
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%% This BibTeX bibliography file was created using BibDesk.
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%% http://bibdesk.sourceforge.net/
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%% Created for Pierre-Francois Loos at 2020-12-03 21:55:19 +0100
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%% Created for Pierre-Francois Loos at 2020-12-04 09:17:19 +0100
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%% Saved with string encoding Unicode (UTF-8)
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@inbook{Lowdin_1958,
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abstract = {Summary This chapter contains sections titled: Introduction Formulation of the Correlation Problem Methods for Treating Electronic Correlation Recent Developments; Concluding Remarks},
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author = {L\"owdin, Per-Olov},
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booktitle = {Adv. Chem. Phys.},
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date-added = {2020-12-04 09:13:16 +0100},
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date-modified = {2020-12-04 09:16:18 +0100},
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doi = {https://doi.org/10.1002/9780470143483.ch7},
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pages = {207-322},
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publisher = {John Wiley \& Sons, Ltd},
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title = {Correlation Problem in Many-Electron Quantum Mechanics I. Review of Different Approaches and Discussion of Some Current Ideas},
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year = {1958},
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Bdsk-Url-1 = {https://onlinelibrary.wiley.com/doi/abs/10.1002/9780470143483.ch7},
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Bdsk-Url-2 = {https://doi.org/10.1002/9780470143483.ch7}}
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@article{Schrodinger_1926,
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author = {Schr{\"o}dinger, E.},
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date-added = {2020-12-03 21:17:40 +0100},
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@ -2302,10 +2316,9 @@
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@article{Wigner_1934,
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author = {Wigner, E.},
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date-modified = {2020-12-04 09:10:54 +0100},
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doi = {10.1103/PhysRev.46.1002},
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journal = {Phys. Rev.},
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month = dec,
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number = {11},
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pages = {1002--1011},
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title = {On the {Interaction} of {Electrons} in {Metals}},
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volume = {46},
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@ -184,7 +184,8 @@ In particular, time-independent Rayleigh--Schr\"odinger perturbation theory \cit
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% Moller-Plesset
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The workhorse of time-independent perturbation theory is most certainly M\o{}ller--Plesset (MP) perturbation
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theory which remains one of the most popular methods for computing the electron correlation energy.\cite{Moller_1934}
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theory \cite{Moller_1934} which remains one of the most popular methods for computing the electron correlation energy,
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an old yet important concept, first introduced by Wigner \cite{Wigner_1934} and later defined by L\"owdin. \cite{Lowdin_1958}
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In this approach, the exact electronic energy is estimated by constructing a perturbative correction on top
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of a mean-field Hartree--Fock (HF) approximation.\cite{SzaboBook}
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The popularity of MP theory stems from its black-box nature and relatively low computational scaling,
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