little paragraph on Olsen 2019

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Pierre-Francois Loos 2020-11-12 15:03:25 +01:00
parent 9217469a29
commit 9672ddc43a
9 changed files with 456 additions and 330 deletions

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@ -55,7 +55,7 @@
\citation{Moller_1934}
\citation{SzaboBook}
\citation{Gill_1994}
\citation{Gill_1986,Gill_1988,Handy_1985,Lepetit_1988}
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\citation{JensenBook}
\citation{Nesbet_1955,Epstein_1926}
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@ -89,10 +89,10 @@
\citation{Sergeev_2005}
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@ -148,34 +148,35 @@
\bibcite{Gill_1988}{{44}{1988}{{Gill\ \emph {et~al.}}}{{Gill, Pople, Radom,\ and\ Nobes}}}
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\bibcite{Lepetit_1988}{{46}{1988}{{Lepetit\ \emph {et~al.}}}{{Lepetit, P{\'e}lissier,\ and\ Malrieu}}}
\bibcite{JensenBook}{{47}{2017}{{Jensen}}{{}}}
\bibcite{Nesbet_1955}{{48}{1955}{{Nesbet\ and\ Hartree}}{{}}}
\bibcite{Epstein_1926}{{49}{1926}{{Epstein}}{{}}}
\bibcite{Seidl_2018}{{50}{2018}{{Seidl\ \emph {et~al.}}}{{Seidl, Giarrusso, Vuckovic, Fabiano,\ and\ Gori-Giorgi}}}
\bibcite{Cremer_1996}{{51}{1996}{{Cremer\ and\ He}}{{}}}
\bibcite{Christiansen_1996}{{52}{1996}{{Christiansen\ \emph {et~al.}}}{{Christiansen, Olsen, J{\o }rgensen, Koch,\ and\ Malmqvist}}}
\bibcite{Sergeev_2005}{{53}{2005}{{Sergeev\ \emph {et~al.}}}{{Sergeev, Goodson, Wheeler,\ and\ Allen}}}
\bibcite{Sergeev_2006}{{54}{2006}{{Sergeev\ and\ Goodson}}{{}}}
\bibcite{Stillinger_2000}{{55}{2000}{{Stillinger}}{{}}}
\bibcite{Baker_1971}{{56}{1971}{{{Baker}}}{{}}}
\bibcite{Goodson_2004}{{57}{2004}{{Goodson\ and\ Sergeev}}{{}}}
\bibcite{Heiss_2002}{{58}{2002}{{Heiss\ and\ M{\"u}ller}}{{}}}
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\bibcite{Cejnar_2005}{{59}{2005}{{Cejnar\ \emph {et~al.}}}{{Cejnar, Heinze,\ and\ Dobe{\v s}}}}
\bibcite{Cejnar_2007}{{60}{2007}{{Cejnar\ \emph {et~al.}}}{{Cejnar, Heinze,\ and\ Macek}}}
\bibcite{Cejnar_2009}{{61}{2009}{{Cejnar\ and\ Jolie}}{{}}}
\bibcite{Borisov_2015}{{62}{2015}{{Borisov\ \emph {et~al.}}}{{Borisov, Ru{\v z}i{\v c}ka,\ and\ Znojil}}}
\bibcite{Sindelka_2017}{{63}{2017}{{{\v S}indelka\ \emph {et~al.}}}{{{\v S}indelka, Santos,\ and\ Moiseyev}}}
\bibcite{Sachdev_2011}{{64}{2011}{{Sachdev}}{{}}}
\bibcite{Cejnar_2015}{{65}{2015}{{Cejnar\ \emph {et~al.}}}{{Cejnar, Str{\'a}nsk{\'y},\ and\ Kloc}}}
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\bibcite{Macek_2019}{{68}{2019}{{Macek\ \emph {et~al.}}}{{Macek, Str{\'a}nsk{\'y}, Leviatan,\ and\ Cejnar}}}
\bibcite{Stransky_2018}{{69}{2018}{{Str{\'a}nsk{\'y}\ \emph {et~al.}}}{{Str{\'a}nsk{\'y}, Dvo{\v r}{\'a}k,\ and\ Cejnar}}}
\bibcite{Lipkin_1965}{{70}{1965}{{Lipkin\ \emph {et~al.}}}{{Lipkin, Meshkov,\ and\ Glick}}}
\bibcite{Cremer_1996}{{52}{1996}{{Cremer\ and\ He}}{{}}}
\bibcite{Christiansen_1996}{{53}{1996}{{Christiansen\ \emph {et~al.}}}{{Christiansen, Olsen, J{\o }rgensen, Koch,\ and\ Malmqvist}}}
\bibcite{Sergeev_2005}{{54}{2005}{{Sergeev\ \emph {et~al.}}}{{Sergeev, Goodson, Wheeler,\ and\ Allen}}}
\bibcite{Sergeev_2006}{{55}{2006}{{Sergeev\ and\ Goodson}}{{}}}
\bibcite{Stillinger_2000}{{56}{2000}{{Stillinger}}{{}}}
\bibcite{Baker_1971}{{57}{1971}{{{Baker}}}{{}}}
\bibcite{Goodson_2004}{{58}{2004}{{Goodson\ and\ Sergeev}}{{}}}
\bibcite{Heiss_2002}{{59}{2002}{{Heiss\ and\ M{\"u}ller}}{{}}}
\bibcite{Cejnar_2005}{{60}{2005}{{Cejnar\ \emph {et~al.}}}{{Cejnar, Heinze,\ and\ Dobe{\v s}}}}
\bibcite{Cejnar_2007}{{61}{2007}{{Cejnar\ \emph {et~al.}}}{{Cejnar, Heinze,\ and\ Macek}}}
\bibcite{Cejnar_2009}{{62}{2009}{{Cejnar\ and\ Jolie}}{{}}}
\bibcite{Borisov_2015}{{63}{2015}{{Borisov\ \emph {et~al.}}}{{Borisov, Ru{\v z}i{\v c}ka,\ and\ Znojil}}}
\bibcite{Sindelka_2017}{{64}{2017}{{{\v S}indelka\ \emph {et~al.}}}{{{\v S}indelka, Santos,\ and\ Moiseyev}}}
\bibcite{Sachdev_2011}{{65}{2011}{{Sachdev}}{{}}}
\bibcite{Cejnar_2015}{{66}{2015}{{Cejnar\ \emph {et~al.}}}{{Cejnar, Str{\'a}nsk{\'y},\ and\ Kloc}}}
\bibcite{Cejnar_2016}{{67}{2016}{{Cejnar\ and\ Str{\'a}nsk{\'y}}}{{}}}
\bibcite{Caprio_2008}{{68}{2008}{{Caprio\ \emph {et~al.}}}{{Caprio, Cejnar,\ and\ Iachello}}}
\bibcite{Macek_2019}{{69}{2019}{{Macek\ \emph {et~al.}}}{{Macek, Str{\'a}nsk{\'y}, Leviatan,\ and\ Cejnar}}}
\bibcite{Stransky_2018}{{70}{2018}{{Str{\'a}nsk{\'y}\ \emph {et~al.}}}{{Str{\'a}nsk{\'y}, Dvo{\v r}{\'a}k,\ and\ Cejnar}}}
\bibcite{Lipkin_1965}{{71}{1965}{{Lipkin\ \emph {et~al.}}}{{Lipkin, Meshkov,\ and\ Glick}}}
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@ -521,6 +521,19 @@
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@ -1,13 +1,28 @@
%% This BibTeX bibliography file was created using BibDesk.
%% http://bibdesk.sourceforge.net/
%% Created for Pierre-Francois Loos at 2020-11-12 10:02:40 +0100
%% Created for Pierre-Francois Loos at 2020-11-12 14:54:07 +0100
%% Saved with string encoding Unicode (UTF-8)
@article{Leininger_2000,
author = {Leininger,Matthew L. and Allen,Wesley D. and Schaefer,Henry F. and Sherrill,C. David},
date-added = {2020-11-12 14:50:57 +0100},
date-modified = {2020-11-12 14:51:07 +0100},
doi = {10.1063/1.481764},
eprint = {https://doi.org/10.1063/1.481764},
journal = {The Journal of Chemical Physics},
number = {21},
pages = {9213-9222},
title = {Is Mo/ller--Plesset perturbation theory a convergent ab initio method?},
url = {https://doi.org/10.1063/1.481764},
volume = {112},
year = {2000},
Bdsk-Url-1 = {https://doi.org/10.1063/1.481764}}
@article{Nesbet_1955,
abstract = { A systematic method is developed for estimating or calculating corrections for configuration interaction in atomic, molecular and nuclear wave-function calculations. Solutions of the Hartree-Fock equations for a single Slater determinant or approximate Hartree-Fock solutions obtained by Roothaan's iterative procedure have special properties which are used to simplify the matrix of the many-particle Hamiltonian. A restricted self-consistent field method is proposed for treating states of low symmetry. This method avoids the off-diagonal Lagrange multipliers encountered in previous methods and is adapted to configuration interaction calculations. },
author = {Nesbet, R. K. and Hartree, Douglas Rayner},
@ -240,17 +255,6 @@
year = {2019},
Bdsk-Url-1 = {https://doi.org/10.1063/1.5110554}}
@article{Leininger_2000,
author = {Leininger, Matthew L. and Allen, Wesley D. and Schaefer, Henry F. and Sherrill, C. David},
date = {2000-05-17},
doi = {10.1063/1.481764},
journal = {J. Chem. Phys.},
number = {21},
pages = {9213--9222},
title = {Is {M{\o}ller-Plesset} perturbation theory a convergent ab initio method?},
volume = {112},
Bdsk-Url-1 = {https://doi.org/10.1063/1.481764}}
@article{Moller_1934,
author = {M{\o}ller, Chr. and Plesset, M. S.},
date = {1934-10-01},

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@ -748,21 +853,21 @@ Class revtex4-1 Warning: Environment acknowledgements is obsolete;
Use acknowledgments instead.
[8]
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@ -1,6 +1,5 @@
\documentclass[aps,prb,reprint,noshowkeys,superscriptaddress]{revtex4-1}
\usepackage{graphicx,dcolumn,bm,xcolor,microtype,multirow,amscd,amsmath,amssymb,amsfonts,physics,longtable,txfonts,mhchem}
\usepackage{graphicx,tabularx,array,booktabs,longtable,dcolumn,xcolor,microtype,multirow,amscd,amsmath,amssymb,amsfonts,physics,siunitx,mhchem}
\usepackage[utf8]{inputenc}
\usepackage[T1]{fontenc}
\usepackage{txfonts}
@ -27,7 +26,6 @@
\newcommand{\fnt}{\footnotetext}
\newcommand{\mcc}[1]{\multicolumn{1}{c}{#1}}
\newcommand{\mr}{\multirow}
\newcommand{\SI}{\textcolor{blue}{supporting information}}
% operators
\newcommand{\bH}{\mathbf{H}}
@ -302,10 +300,10 @@ with $\mel{pq}{}{rs} = \braket{pq}{rs} - \braket{pq}{sr}$, and where
\begin{equation}
\braket{pq}{rs} = \iint \dd\vb{x}_1\dd\vb{x}_2\frac{\phi_p(\vb{x}_1)\phi_q(\vb{x}_2)\phi_r(\vb{x}_1)\phi_s(\vb{x}_2)}{\abs{\vb{r}_1 - \vb{r}_2}}
\end{equation}
are two-electron integral in the spin-orbital basis. \cite{Gill_1994}
are two-electron integrals in the spin-orbital basis. \cite{Gill_1994}
As mentioned earlier, there is, \textit{a priori}, no guarantee that the MP$m$ series converges to the exact energy when $m \to \infty$.
In fact, it is known that when the HF wave function is a poor approximation to the exact wave function, for example in multi-reference systems, the MP method yields deceptive results. \cite{Gill_1986, Gill_1988, Handy_1985, Lepetit_1988}
In fact, it is known that when the HF wave function is a poor approximation to the exact wave function, for example in multi-reference systems, the MP method yields deceptive results. \cite{Gill_1986,Gill_1988,Handy_1985,Lepetit_1988,Leininger_2000}
A convenient way to investigate the convergence properties of the MP series is to analytically continue the coupling parameter $\lambda$ into the complex variable.
By doing so, the Hamiltonian and the energy become complex-valued functions of $\lambda$, and the energy becomes a multivalued function on $K$ Riemann sheets (where $K$ is the number of basis functions).
As mentioned above, by searching the singularities of the function $E(\lambda)$, one can get information on the convergence properties of the MP series.
@ -364,11 +362,16 @@ The discovery of this divergent behavior is worrying as in order to get meaningf
A singularity in the unit circle is designated as an intruder state, more precisely as a front-door (respectively back-door) intruder state if the real part of the singularity is positive (respectively negative). Their method consists in performing a scan of the real axis to detect the avoided crossing responsible for the pair of dominant singularities. Then, by modeling this avoided crossing via a two-state Hamiltonian one can get an approximation of the dominant conjugate pair of singularities by finding the EPs of the following $2\times2$ matrix
\begin{equation}
\underbrace{\mqty(\alpha & \delta \\ \delta & \beta)}_{\bH} = \underbrace{\mqty(\alpha + \alpha_s & 0 \\ 0 & \beta + \beta_s )}_{\bH^{(0)}} + \underbrace{\mqty(- \alpha_s & \delta \\ \delta & - \beta_s)}_{\bV},
\underbrace{\mqty(\alpha & \delta \\ \delta & \beta)}_{\bH} = \underbrace{\mqty(\alpha & 0 \\ 0 & \beta + \gamma )}_{\bH^{(0)}} + \underbrace{\mqty( 0 & \delta \\ \delta & - \gamma)}_{\bV},
\end{equation}
where the diagonal matrix is the unperturbed Hamiltonian matrix $\bH^{(0)}$ and the second matrix in the right-hand-side $\bV$ is the perturbation.
In Ref.~\onlinecite{Olsen_2019}, the simple $2 \times 2$ model proposed by Olsen \textit{et al.} is generalized to a non-symmetric (i.e, non-Hermitian) Hamiltonian and various choice of perturbation (not only the MP partioning).
In Ref.~\onlinecite{Olsen_2019}, the simple two-state model proposed by Olsen \textit{et al.} is generalized to a non-symmetric Hamiltonian
\begin{equation}
\underbrace{\mqty(\alpha & \delta_1 \\ \delta_2 & \beta)}_{\bH} = \underbrace{\mqty(\alpha & 0 \\ 0 & \beta + \gamma )}_{\bH^{(0)}} + \underbrace{\mqty( 0 & \delta_2 \\ \delta_1 & - \gamma)}_{\bV}.
\end{equation}
allowing an analysis of various choice of perturbation (not only the MP partioning) such as coupled cluster perturbation expansions and other non-Hermitian perturbation methods.
It is worth noting that only cases where $\text{sgn}(\delta_1) = - \text{sgn}(\delta_2)$ leads to new forms of perturbation expansions.
Interestingly, they showed that the convergence pattern of a given perturbation method can be characterized by its archetype which defines the overall ``shape'' of the energy convergence and can be subdivided in five classes for Hermitian Hamiltonians (zigzag, interspersed zigzag, triadic, ripples, and geometric), while two additional archetypes (zigzag-geometric and convex-geometric) are observed in non-Hermitian Hamiltonians.
Other features characterizing the convergence behavior of a perturbation method are its rate of convergence, its length of recurring period, and its sign pattern.

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