From 35e5dbbc0833537b0a711ff257a55e16df1b8824 Mon Sep 17 00:00:00 2001
From: Hugh Burton <hb407@cam.ac.uk>
Date: Thu, 19 Nov 2020 12:14:23 +0000
Subject: [PATCH] minor edit

---
 Manuscript/EPAWTFT.tex | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

diff --git a/Manuscript/EPAWTFT.tex b/Manuscript/EPAWTFT.tex
index 81ff516..1f0823e 100644
--- a/Manuscript/EPAWTFT.tex
+++ b/Manuscript/EPAWTFT.tex
@@ -484,7 +484,7 @@ the spin-$\sigma$ electrons as
 In the weak correlation regime $0 \le U \le 2t$, the angles which minimise the HF energy, 
 \ie, $\pdv*{E_\text{HF}}{\theta_\sigma} = 0$, are 
 \begin{equation}
-	\ta^\text{RHF} = \tb^\text{RHF} = \pi/4,
+	\ta^\text{RHF} = \tb^\text{RHF} = \pi/2,
 \end{equation}
 giving the symmetry-pure molecular orbitals
 \begin{align}