From 5b989cf206023ae5c7585b841bd2300d4abba4c2 Mon Sep 17 00:00:00 2001
From: eginer <giner.emmanuel@gmail.com>
Date: Fri, 6 Dec 2019 16:36:53 +0100
Subject: [PATCH] minor modifs on t2's modifs on the effective operator

---
 JCTC_revision/GW-srDFT.tex | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

diff --git a/JCTC_revision/GW-srDFT.tex b/JCTC_revision/GW-srDFT.tex
index f08e038..763f8cb 100644
--- a/JCTC_revision/GW-srDFT.tex
+++ b/JCTC_revision/GW-srDFT.tex
@@ -483,7 +483,7 @@ where, in the case of a single-determinant method (such as HF and KS-DFT),}
 \end{equation}
 and 
 \begin{equation}
-	\n{2}{\Bas}(\br{}) = n_{\uparrow}^{\Bas}(\br{}) n_{\downarrow}^{\Bas}(\br{}')
+	\n{2}{\Bas}(\br{},\br{}') = n_{\uparrow}^{\Bas}(\br{}) n_{\downarrow}^{\Bas}(\br{}')
 \end{equation}
 is the opposite-spin pair density in a closed-shell system.