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\newcommand { \LCPQ } { Laboratoire de Chimie et Physique Quantiques (UMR 5626), Universit\' e de Toulouse, CNRS, UPS, France}
\newcommand { \LCT } { Laboratoire de Chimie Th\' eorique, Universit\' e Pierre et Marie Curie, Sorbonne Universit\' e, CNRS, Paris, France}
\begin { document}
\title { G2 Atomization Energies With Chemical Accuracy}
\author { Bath\' elemy Pradines}
\affiliation { \LCPQ }
\author { Anthony Scemama}
\affiliation { \LCPQ }
\author { Julien Toulouse}
\affiliation { \LCT }
\author { Pierre-Fran\c { c} ois Loos}
\email [Corresponding author: ] { loos@irsamc.ups-tlse.fr}
\affiliation { \LCPQ }
\author { Emmanuel Giner}
\affiliation { \LCT }
\begin { abstract}
\end { abstract}
\maketitle
%%%%%%%%%%%%%%%%%%%%%%%%
\section { Introduction}
%%%%%%%%%%%%%%%%%%%%%%%%
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%%%%%%%%%%%%%%%%%%%%%%%%
\section { Theory}
%%%%%%%%%%%%%%%%%%%%%%%%
\subsection { The DFT basis-set correction in a nutshell}
The basis-set correction investigated here proposes to use the RSDFT formalism to capture a part of the short-range correlation effects missing in a finite one-electron basis-set.
In a nutshell, this formalism relies on 1) the definition of a complementary density functional aiming at describing the correlation effects absent in a finite basis-set, 2) the definition of an \textit { effective non divergent interaction} as the real-space representation of the coulomb operator projected in a finite basis-set,
3) the fit of such an effective interaction with a long-range interaction through the definition of a \textit { range-separation parameter varying in space} , 4) the use of a correlation functional from RSDFT with a \textit { multi-determinant} reference evaluated with the range-separation parameter varying in space.
More details can be found in \cite { GinPraFerAssSavTou-JCP-18} .
\subsubsection { Definition of basis-set dependent complementary functional}
The
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%%%%%%%%%%%%%%%%%%%%%%%%
\section { Results}
%%%%%%%%%%%%%%%%%%%%%%%%
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\subsection { The case of C$ _ 2 $ and the comparison with the F12 methods.}
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\begin { table*}
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\caption { Dissociation energy ($ D _ e $ ) in kcal/mol of the F$ _ 2 $ molecule computed using FCIQMC, CIPSI, FCIQMC+F$ _ { 12 } $ , CIPSI+LDA$ _ { \rm HF } $ and CIPSI+LDA$ _ { \text { HF - val } } $ (valence only interaction and density) in the Dunnng cc-pVXZ (VXZ) basis sets. $ ^ a $ Results from Ref\cite { PetTouUmr-JCP-12} taking into account the ZPE correction. }
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\begin { ruledtabular}
\begin { tabular} { lccccc}
%\hline
& CIPSI & CIPSI+LDA$ _ { \text { HF } } $ & CIPSI+LDA$ { _ \text { HF - val } } $ & CIPSI+PBE$ _ { \text { HF } } $ & CIPSI+PBE$ { _ \text { HF - val } } $ \\
\hline
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V2Z & 27.5 & 30.8 & 31.1 & 32.1 & 32.4 \\
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V3Z & 35.4 & 37.0 & 37.5 & 37.5 & 37.8 \\
V4Z & 37.5 & 38.7 & 38.8 & 38.7 & 38.8 \\
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V5Z & 38.0 & 38.7 & 38.8 & 38.7 & 38.8 \\
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%\hline
& \multicolumn { 5} { c} { Estimated exact} \\
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& \multicolumn { 5} { c} { 38.2$ ^ a $ } \\
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\end { tabular}
\end { ruledtabular}
\label { conv_ He_ table}
\end { table*}
\begin { table*}
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\caption {
\label { tab:diatomics}
Dissociation energy ($ \De $ ) in kcal/mol of the \ce { C2} , \ce { O2} , \ce { N2} and \ce { F2} molecules computed with various methods and basis sets.
}
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\begin { ruledtabular}
\begin { tabular} { llddddd}
& & \mc { 4} { c} { Dunning's basis set}
\\
\cline { 3-6}
Molecule & Method & \tabc { cc-pVDZ} & \tabc { cc-pVTZ} & \tabc { cc-pVQZ} & \tabc { cc-pV5Z} & \tabc { Exp.}
\\
\hline
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\ce { C2} & FCIQMC & 130.0(1) & 139.9(3) & 143.3(2) & & 146.9(5)\fnm [1] \\
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& FCIQMC+F12 & 142.3 & 145.3 & & & \\
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\hline
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& exFCI & 132.0 & 140.3 & 143.6 & 144.3 & \\
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\hline
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& exFCI+LDA & 141.9 & 142.8 & 145.8 & 146.2 & \\
& exFCI+LDA(FC) & 142.9 & 145.5 & 146.2 & 146.1 & \\
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\hline
& exFCI+PBE & 146.1 & 143.9 & 145.9 & 145.12 & \\
& exFCI+PBE (FC) & 147.7 & 146.3 & 146.4 & 146.0 & \\
\hline
& exFCI+PBE-on-top& 142.7 & 142.7 & 145.3 & 144.9 & \\
& exFCI+PBE-on-top(FC) & 143.3 & 144.7 & 145.7 & 145.6 & \\
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\\
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\ce { N2} & exFCI & 200.9 & 217.1 & 223.5 & 225.7 & 228.5\fnm [2] \\
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\hline
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& exFCI+LDA & 216.3 & 223.1 & 227.9 & 227.9 & \\
& exFCI+LDA(FC) & 218.2 & 225.8 & 228.8 & 228.4 & \\
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\hline
& exFCI+PBE & 225.3 & 225.6 & 228.2 & 227.9 & \\
& exFCI+PBE (FC) & 228.6 & 228.1 & 228.9 & 228.6 & \\
\hline
& exFCI+PBE-on-top& 222.3 & 224.6 & 227.7 & 227.7 & \\
& exFCI+PBE-on-top(FC) & 224.8 & 226.7 & 228.3 & 228.3 & \\
\\
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\ce { O2} & exFCI & 105.3 & 114.6 & 118.0 & 119.1 & 120.2\fnm [2] \\
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\hline
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& exFCI+LDA & 111.8 & 117.2 & 120.0 & 119.9 & \\
& exFCI+LDA(FC) & 112.5 & 118.5 & 120.2 & 120.2 & \\
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\hline
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& exFCI+PBE & 115.9 & 118.4 & 120.1 & 119.9 & \\
& exFCI+PBE (FC) & 117.5 & 119.5 & 120.4 & 120.3 & \\
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\hline
& exFCI+PBE-on-top& 115.0 & 118.4 & 120.2 & & \\
& exFCI+PBE-on-top(FC) & 116.1 & 119.4 & 120.5 & & \\
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\\
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\ce { F2} & exFCI & 27.5 & 35.4 & 37.5 & 38.0 & 38.2\fnm [2] \\
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\hline
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& exFCI+LDA & 30.8 & 37.0 & 38.7 & 38.7 & \\
& exFCI+LDA(FC) & 31.1 & 37.5 & 38.8 & 38.8 & \\
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\hline
& exFCI+PBE & 33.3 & 37.8 & 38.8 & 38.7 & \\
& exFCI+PBE (FC) & 33.9 & 38.2 & 39.0 & 38.8 & \\
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\hline
& exFCI+PBE-on-top& 32.1 & 37.5 & 38.7 & 38.7 & \\
& exFCI+PBE-on-top(FC) & 32.4 & 37.8 & 38.8 & 38.8 & \\
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\end { tabular}
\end { ruledtabular}
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\fnt [1] { Results from Ref.~\onlinecite { BytLaiRuedenJCP05} .}
\fnt [2] { Results from Ref.~\onlinecite { PetTouUmr-JCP-12} .}
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\end { table*}
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%
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\bibliography { G2-srDFT}
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\end { document}