diff --git a/Manuscript/G2-srDFT.bib b/Manuscript/G2-srDFT.bib
index b541937..8e17c3f 100644
--- a/Manuscript/G2-srDFT.bib
+++ b/Manuscript/G2-srDFT.bib
@@ -4508,6 +4508,7 @@
 
 @article{GolWerSto-PCCP-05,
 	Author = {Erich Goll and Hans-Joachim Werner and Hermann Stoll},
+        title = {A short-range gradient-corrected density functional in long-range coupled-cluster calculations for rare gas dimers},
 	Journal = {Phys. Chem. Chem. Phys.},
 	Pages = {3917},
 	Volume = {7},
@@ -5871,6 +5872,7 @@
 
 @article{JanHenScu-JCP-09,
 	Author = {B. G. Janesko and T. M. Henderson and G. E. Scuseria},
+        title = {Long-range-corrected hybrids including random phase approximation correlation},
 	Journal = {J. Chem. Phys.},
 	Pages = {081105},
 	Volume = {130},
@@ -12212,7 +12214,7 @@
 	Author = {Holmes,Adam A. and Umrigar,C. J. and Sharma,Sandeep},
 	Doi = {10.1063/1.4998614},
 	Eprint = {https://doi.org/10.1063/1.4998614},
-	Journal = {The Journal of Chemical Physics},
+	Journal = {J. Chem. Phys.},
 	Number = {16},
 	Pages = {164111},
 	Title = {Excited states using semistochastic heat-bath configuration interaction},
@@ -12269,7 +12271,7 @@
 	Author = {Dasgupta, Saswata and Herbert, John M.},
 	Doi = {10.1002/jcc.24761},
 	Eprint = {https://onlinelibrary.wiley.com/doi/pdf/10.1002/jcc.24761},
-	Journal = {Journal of Computational Chemistry},
+	Journal = {J. Comput. Chem.},
 	Number = {12},
 	Pages = {869-882},
 	Title = {Standard grids for high-precision integration of modern density functionals: SG-2 and SG-3},
@@ -12279,7 +12281,7 @@
 
 @article{Tenno-CPL-04,
 title = "Initiation of explicitly correlated Slater-type geminal theory",
-journal = "Chemical Physics Letters",
+journal = "Chem. Phys. Lett.",
 volume = "398",
 number = "1",
 pages = "56 - 61",
diff --git a/Manuscript/G2-srDFT.tex b/Manuscript/G2-srDFT.tex
index c46ab51..a0cf2ad 100644
--- a/Manuscript/G2-srDFT.tex
+++ b/Manuscript/G2-srDFT.tex
@@ -390,11 +390,11 @@ Depending on the functional choice, the complementary functional $\bE{}{\Bas}[\n
 As most WFT calculations are performed within the frozen-core (FC) approximation, it is important to define an effective interaction within a subset of MOs. 
 We then naturally split the basis set as $\Bas = \Cor \bigcup \BasFC$ (where $\Cor$ and $\BasFC$ are the sets of core and active MOs, respectively) and define the FC version of the effective interaction as
  \begin{equation}
-	\W{\Bas}{\FC}(\br{1},\br{2})  = 
+	\W{\Bas}{\FC}(\br{1},\br{2})  \! = \!
     \begin{cases}
-	\f{\Bas}{\FC}(\br{1},\br{2})/\n{2,\Bas}{\FC}(\br{1},\br{2}),  & \text{if $\n{2,\Bas}{\FC}(\br{1},\br{2})\ne 0$},
+	\f{\Bas}{\FC}(\br{1},\br{2})/\n{2,\Bas}{\FC}(\br{1},\br{2}),\!  & \!\!\! \text{if $\n{2,\Bas}{\FC}(\br{1},\br{2}) \!\ne \! 0$},
 	\\
-	\infty, & \text{otherwise,}
+	\infty, \! & \!\!\! \text{otherwise,}
     \end{cases}
  \end{equation}
 with 
@@ -512,7 +512,7 @@ To estimate the CBS limit of each method, following Ref.~\onlinecite{HalHelJorKl
 
 As the exFCI calculations are converged with a precision of about 0.1 {\kcal} on atomization energies, we can label those as near-FCI. 
 Hence, they will be our references for \ce{C2}, \ce{N2}, \ce{O2} and \ce{F2}. 
-The results for these diatomics are reported in Fig.~\ref{fig:diatomics}. 
+The results for these diatomic molecules are reported in Fig.~\ref{fig:diatomics}. 
 The corresponding numerical data can be found in the {\SI}.
 As one can see, the convergence of the exFCI atomization energies is, as expected, slow with respect to the basis set: chemical accuracy (error below 1 {\kcal}) is barely reached for \ce{C2}, \ce{O2} and \ce{F2} even with the cc-pV5Z basis set, and the atomization energies are consistently underestimated.
 A similar trend holds for CCSD(T).
@@ -545,7 +545,7 @@ Encouraged by these promising results, we are currently pursuing various avenues
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \section*{Supporting information}
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
-See {\SI} for raw data associated with the atomization energies of the four diatomics and the G2 set.
+See {\SI} for raw data associated with the atomization energies of the four diatomic molecules and the G2 set.
 
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \begin{acknowledgements}