correction Mika
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@ -359,7 +359,7 @@ More details can be found in Ref.~\onlinecite{Nocedal_1999}.
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%%% TABLE I %%%
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\begin{squeezetable}
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\begin{table*}
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\caption{Total energy $E$ (in \SI{}{\hartree}) and correlation energy $\Delta E$ (in \SI{}{\milli\hartree}) for the frozen-core ground state of five-membered rings in the cc-pVDZ basis set.
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\caption{Total energy $E$ (in \si{\hartree}) and correlation energy $\Delta E$ (in \si{\milli\hartree}) for the frozen-core ground state of five-membered rings in the cc-pVDZ basis set.
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For the CIPSI estimates of the FCI correlation energy, the fitting error associated with the weighted five-point linear fit is reported in parenthesis.
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\label{tab:Tab5-VDZ}}
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\begin{ruledtabular}
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@ -398,7 +398,7 @@ More details can be found in Ref.~\onlinecite{Nocedal_1999}.
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%%% TABLE II %%%
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\begin{squeezetable}
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\begin{table*}
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\caption{Total energy $E$ (in \SI{}{\hartree}) and correlation energy $\Delta E$ (in \SI{}{\milli\hartree}) for the frozen-core ground state of six-membered rings in the cc-pVDZ basis set.
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\caption{Total energy $E$ (in \si{\hartree}) and correlation energy $\Delta E$ (in \si{\milli\hartree}) for the frozen-core ground state of six-membered rings in the cc-pVDZ basis set.
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For the CIPSI estimates of the FCI correlation energy, the fitting error associated with the weighted five-point linear fit is reported in parenthesis.
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\label{tab:Tab6-VDZ}}
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\begin{ruledtabular}
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@ -437,7 +437,7 @@ More details can be found in Ref.~\onlinecite{Nocedal_1999}.
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\begin{squeezetable}
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\begin{table}
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\caption{
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Extrapolated correlation energies $\Delta \Eextrap$ (in \SI{}{\milli\hartree}) for the twelve cyclic molecules represented in Fig.~\ref{fig:mol} and their associated fitting errors (in \SI{}{\milli\hartree}) obtained via weighted linear fits with a varying number of points.
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Extrapolated correlation energies $\Delta \Eextrap$ (in \si{\milli\hartree}) for the twelve cyclic molecules represented in Fig.~\ref{fig:mol} and their associated fitting errors (in \si{\milli\hartree}) obtained via weighted linear fits with a varying number of points.
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Two sets of orbitals are considered: natural orbitals and optimized orbitals.
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The weights are taken as the inverse square of the perturbative corrections.
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For a $m$-point fit, the $m$ largest variational wave functions are used.
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@ -552,7 +552,7 @@ More details can be found in Ref.~\onlinecite{Nocedal_1999}.
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\includegraphics[width=0.32\textwidth]{Pyrimidine_MPCC}
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\includegraphics[width=0.32\textwidth]{Tetrazine_MPCC}
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\includegraphics[width=0.32\textwidth]{Triazine_MPCC}
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\caption{Convergence of the correlation energy (in \SI{}{\milli\hartree}) as a function of the computational cost for the twelve cyclic molecules represented in Fig.~\ref{fig:mol}.
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\caption{Convergence of the correlation energy (in \si{\milli\hartree}) as a function of the computational cost for the twelve cyclic molecules represented in Fig.~\ref{fig:mol}.
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Three series of methods are considered: i) MP2, MP3, MP4, and MP5 (blue), ii) CC2, CC3, and CC4 (green), and iii) CCSD, CCSDT, CCSDTQ (red).
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The FCI estimate of the correlation energy is represented as a black line.
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\label{fig:MPCC}}
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@ -563,7 +563,7 @@ More details can be found in Ref.~\onlinecite{Nocedal_1999}.
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\begin{squeezetable}
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\begin{table}
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\caption{
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Mean absolute error (MAE), mean signed error (MSE), and minimum (Min) and maximum (Max) absolute errors (in \SI{}{\milli\hartree}) with respect to the FCI correlation energy for various methods.
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Mean absolute error (MAE), mean signed error (MSE), and minimum (Min) and maximum (Max) absolute errors (in \si{\milli\hartree}) with respect to the FCI correlation energy for various methods.
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The formal computational scaling of each method is also reported.
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\label{tab:stats}}
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\begin{ruledtabular}
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@ -623,7 +623,7 @@ Each Irene's AMD node is a dual-socket AMD Rome (EPYC) CPU at 2.60 GHz with 256G
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These nodes are connected via Infiniband HDR100.
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In total, the present calculations have required around 3~million core hours.
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All the data (geometries, energies, etc) and supplementary material associated with the present manuscript are openly available in Zenodo at \href{http://doi.org/XX.XXXX/zenodo.XXXXXXX}{http://doi.org/XX.XXXX/zenodo.XXXXXXX}.
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All the data (geometries, energies, etc) and supplementary material associated with the present manuscript are openly available in Zenodo at \url{http://doi.org/XX.XXXX/zenodo.XXXXXXX}.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Results and discussion}
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@ -723,7 +723,7 @@ This project has received funding from the European Research Council (ERC) under
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%%%%%%%%%%%%%%%%%%%%%%%%%
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\section*{Data availability statement}
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%%%%%%%%%%%%%%%%%%%%%%%%%
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The data that support the findings of this study are openly available in Zenodo at \href{http://doi.org/XX.XXXX/zenodo.XXXXXXX}{http://doi.org/XX.XXXX/zenodo.XXXXXXX}.
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The data that support the findings of this study are openly available in Zenodo at \url{http://doi.org/XX.XXXX/zenodo.XXXXXXX}.
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%%%%%%%%%%%%%%%%%%%%%%%%%
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\bibliography{Ec}
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