results section

Manuscript/G2-srDFT.tex

@@ -569,17 +569,18 @@ Importantly, the sensitivity with respect to the SR-DFT functional is quite larg
 However, from the quadruple-$\zeta$ basis, the LDA and PBE functionals agree within a few tenths of a {\kcal}. 
 Such weak sensitivity to the approximated functionals in the DFT part when reaching large basis sets shows the robustness of the approach. 
 
-We have computed the correlation energies of the G2-1 test sets with $\modY=\CCSDT$, $\modZ=\HF$ and the cc-pVXZ basis.
+We have computed the correlation energies of the G2-1 test sets with $\modY=\CCSDT$, $\modZ=\HF$ and the cc-pVXZ basis sets.
-The plain CCSD(T) correlation energies as well as the corrected CCSD(T)+LDA and CCSD(T)+PBE values are reported.
+The ``plain'' CCSD(T) correlation energies as well as the corrected CCSD(T)+LDA and CCSD(T)+PBE values are depicted in Fig.~\ref{fig:G2_Ec}.
-A statistical analysis of these data is also provided in Table \ref{tab:stats}, where one can find the mean absolute deviation (MAD), the root-mean-square deviation (RMSD), and the maximum deviation (MAX) with respect to the CCSD(T)/CBS reference correlation energies.
+The raw data can be found in the {\SI}.
+A statistical analysis of these data is also provided in Table \ref{tab:stats}, where we have reported the mean absolute deviation (MAD), root-mean-square deviation (RMSD), and maximum deviation (MAX) with respect to the CCSD(T)/CBS correlation energies.
 From double-$\zeta$ to quintuple-$\zeta$ basis, the MAD associated with the CCSD(T) correlation energies goes down slowly from 14.29 to 1.28 {\kcal}.
-For typical basis like cc-pVTZ, the MAD of CCSD(T) is still 6.06 {\kcal}.
+For a commonly-used basis like cc-pVTZ, the MAD of CCSD(T) is still 6.06 {\kcal}.
 Applying the basis set correction drastically reduces the basis set incompleteness error.
 Already at the CCSD(T)+LDA/cc-pVDZ and CCSD(T)+PBE/cc-pVDZ levels, the MAD is reduced to 3.24 and 1.96 {\kcal}.
-With the triple-$\zeta$ basis, the CCSD(T)+PBE/cc-pVTZ are already below 1 {\kcal} with 36 cases (out of 55) where we achieve chemical accuracy.
+With the triple-$\zeta$ basis, the MAD of CCSD(T)+PBE/cc-pVTZ is already below 1 {\kcal} with 36 cases (out of 55) where we achieve chemical accuracy.
 CCSD(T)+LDA/cc-pVQZ and CCSD(T)+PBE/cc-pVQZ return MAD of 0.33 and 0.31 kcal/mol (respectively) while CCSD(T)/cc-pVQZ still yields a fairly large MAD of 2.50 {\kcal}.
 
-Therefore, similarly to F12 methods, \cite{TewKloNeiHat-PCCP-07} we can safely claim that the present basis set correction recover quintuple-$\zeta$ quality coupled-cluster correlation energies with triple-$\zeta$ basis sets for a much cheaper computational cost.
+Therefore, similar to F12 methods, \cite{TewKloNeiHat-PCCP-07} we can safely claim that the present basis set correction recovers quintuple-$\zeta$ quality correlation energies with triple-$\zeta$ basis sets for a much cheaper computational cost.
 
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \section*{Supporting information}