JCP version for ref

Manuscript/CI-F12.tex

@@ -1,4 +1,4 @@
-\documentclass[aip,jcp,reprint,showkeys]{revtex4-1}
+\documentclass[aip,jcp,reprint]{revtex4-1}
 \usepackage{graphicx,dcolumn,bm,xcolor,microtype,hyperref,multirow,amscd,amsmath,amssymb,amsfonts,physics,mhchem}
 \usepackage{mathpazo,libertine}
 \newcommand{\alert}[1]{\textcolor{red}{#1}}
@@ -78,7 +78,7 @@ This greatly enhances the convergence with respect to the one-electron basis set
 The performance of the newly-designed explicitly-correlated CI-F12 method is illustrated on atoms and molecules.
 \end{abstract}
 
-\keywords{configuration interaction; explicitly-correlated methods; effective Hamiltonian theory}
+%\keywords{configuration interaction; explicitly-correlated methods; effective Hamiltonian theory}
 
 \maketitle
 
@@ -89,7 +89,7 @@ The performance of the newly-designed explicitly-correlated CI-F12 method is ill
 	\textit{``The key idea is that traditional CI is not really bad, it only has difficulties to represent the wave function at those regions of configuration space where one interelectronic distance $r_{ij}$ approaches zero.''}
 	\flushright --- Werner Kutzelnigg, 
 	\\
-	\textit{Theor.~Chim.~Acta} (1985) \textbf{68} 445--469.
+	\textit{Theor.~Chim.~Acta} \textbf{68} (1985) 445--469.
 \end{quotation}
 One of the most fundamental and severe error in electronic structure methods is the (one-electron) basis set incompleteness.
 In particular, conventional quantum chemistry wave function methods typically display a slow energy convergence with respect to the size of the one-electron basis set.