From af9198832a6928147e33344bb12a0271d52e690e Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Sun, 28 May 2023 12:21:56 +0200
Subject: Removed of course

---
 2-point.tex | 10 +++++-----
 1 file changed, 5 insertions(+), 5 deletions(-)

(limited to '2-point.tex')

diff --git a/2-point.tex b/2-point.tex
index d02fbfd..2c61253 100644
--- a/2-point.tex
+++ b/2-point.tex
@@ -729,11 +729,11 @@ and a specific realization of the disordered Hamiltonian is
 \end{equation}
 where the first $\delta$-function keeps the configurations in the tangent
 plane, and the second enforces the spherical constraint. We have anticipated
-treating the logarithm with replicas. We are of course interested in
-points $\mathbf s$ that have certain properties: they are stationary points of
-$H$ with given energy density and stability, and fixed overlap from a reference
-configuration $\pmb\sigma$. We therefore average the free energy above over
-such points, giving
+treating the logarithm with replicas. We are interested in points $\mathbf s$
+that have certain properties: they are stationary points of $H$ with given
+energy density and stability, and fixed overlap from a reference configuration
+$\pmb\sigma$. We therefore average the free energy above over such points,
+giving
 \begin{equation}
   \begin{aligned}
     F_H(\beta\mid E_1,\mu_1,q,\pmb\sigma)
-- 
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