saving work in results

BSEdyn.tex

@@ -744,7 +744,7 @@ All the static and dynamic BSE calculations have been performed with the softwar
 %%% TABLE I %%%
 \begin{table*}
 	\caption{
-	Singlet and triplet excitation energies (in eV) of \ce{N2} at the BSE@{\GOWO}@HF level for various basis sets.
+	Singlet and triplet excitation energies (in eV) of \ce{N2} computed at the BSE@{\GOWO}@HF level for various basis sets.
 	\label{tab:N2}
 	}
 	\begin{ruledtabular}
@@ -773,13 +773,19 @@ All the static and dynamic BSE calculations have been performed with the softwar
 	\end{ruledtabular}
 \end{table*}
 
+First, we investigate the basis set dependency of the dynamical correction as well as the validity of the dTDA (which corresponds to neglecting the dynamical correction originating from the anti-resonant part of the BSE Hamiltonian). 
+Note that, in the present calculations, the zeroth-order Hamiltonian is always the ``full'' BSE static Hamiltonian, \ie, without TDA.
+The singlet and triplet excitation energies of the nitrogen molecule \ce{N2} computed at the BSE@{\GOWO}@HF level for the aug-cc-pVDZ, aug-cc-pVTZ, and aug-cc-pVQZ basis sets are reported in Table \ref{tab:N2}, where we also report the $GW$ gap, $\Eg^{\GW}$, to show that each corrected transition is well below this gap.
+The \ce{N2} molecule is a very convenient example as it contains $n \ra \pis$ and $\pi \ra \pis$ valence excitations as well as Rydberg transitions.
+As we shall see later, the magnitude of the dynamical correction is characteristic of the type of transitions.
+
 
 %%% TABLE I %%%
 %\begin{squeezetable}
 \begin{table*}
 	\caption{
-	Singlet excitation energies (in eV) for various molecules obtained with the aug-cc-pVTZ basis set at various levels of theory.
-	The dynamical correction is computed in the TDA.
+	Singlet excitation energies (in eV) for various molecules obtained with the aug-cc-pVTZ basis set computed at various levels of theory.
+	The dynamical correction is computed in the dTDA.
 	CT and R stand respectively for charge transfer and Rydberg.
 	\label{tab:BigTabSi}
 	}
@@ -861,8 +867,8 @@ All the static and dynamic BSE calculations have been performed with the softwar
 %\begin{squeezetable}
 \begin{table*}
 	\caption{
-	Triplet excitation energies (in eV) for various molecules obtained with the aug-cc-pVTZ basis set at various levels of theory.
-	The dynamical correction is computed in the TDA.
+	Triplet excitation energies (in eV) for various molecules obtained with the aug-cc-pVTZ basis set computed at various levels of theory.
+	The dynamical correction is computed in the dTDA.
 	\label{tab:BigTabTr}
 	}
 	\begin{ruledtabular}