From fbea44ea732b938ec34ed6f95b9b7c16f874f33c Mon Sep 17 00:00:00 2001
From: Pierre-Francois Loos <pierrefrancois.loos@gmail.com>
Date: Mon, 3 Feb 2020 16:30:00 +0100
Subject: [PATCH] conflicts

---
 BSE-PES.tex | 2 --
 1 file changed, 2 deletions(-)

diff --git a/BSE-PES.tex b/BSE-PES.tex
index 38b8f03..e4c2da5 100644
--- a/BSE-PES.tex
+++ b/BSE-PES.tex
@@ -347,7 +347,6 @@ In Eq.~\eqref{eq:W},  $\eta$ is a positive infinitesimal, and $\OmRPA{m}{\IS}$ a
 \begin{subequations}
 \label{eq:LR_RPA}
 \begin{align}
-	\label{eq:LR_RPA}
 	\ARPA{ia,jb}{\IS} & = \delta_{ij} \delta_{ab} (\eHF{a} - \eHF{i}) +   2 \IS \ERI{ia}{jb},
 	\\ 
 	\BRPA{ia,jb}{\IS} & =   2 \IS \ERI{ia}{bj},
@@ -361,7 +360,6 @@ so that   $W^{\lambda}$ reduces to the bare Coulomb potential. In that limit,  t
 \begin{subequations}
 \label{eq:LR_RPAx}
 \begin{align}
-	\label{eq:LR_RPAx}
 	\ARPAx{ia,jb}{\IS} & = \delta_{ij} \delta_{ab} (\eHF{a} - \eHF{i}) + \IS \qty[ 2 \ERI{ia}{jb} -    \ERI{ij}{ab} ],
 	\\ 
 	\BRPAx{ia,jb}{\IS} & =  \IS \qty[ 2 \ERI{ia}{bj} - \ERI{ib}{aj} ].