From 7569d4b2ae6e519eab8d3398b804c32c9bb64ad8 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Wed, 18 Sep 2024 22:29:52 +0200
Subject: Small tweaks.

---
 topology.tex | 6 +++---
 1 file changed, 3 insertions(+), 3 deletions(-)

(limited to 'topology.tex')

diff --git a/topology.tex b/topology.tex
index bbd978a..127b15e 100644
--- a/topology.tex
+++ b/topology.tex
@@ -78,7 +78,7 @@ out-of-equilibrium dynamics.
 % This block will be filled during the proof stage, and finilized just before publication.
 % It exists here only as a placeholder, and should not be modified by authors.
 \noindent\textcolor{white!90!black}{%
-\fbox{\parbox{0.975\linewidth}{%
+\fbox{\parbox{0.972\linewidth}{%
 \textcolor{white!40!black}{\begin{tabular}{lr}%
   \begin{minipage}{0.6\textwidth}%
     {\small Copyright attribution to authors. \newline
@@ -244,8 +244,8 @@ the sign of the determinant, we arrive at the Euler characteristic, or
   \chi(\Omega)=\int_\Omega d\mathbf x\,\delta\big(\nabla H(\mathbf x)\big)\det\operatorname{Hess}H(\mathbf x)
 \end{equation}
 When the Kac--Rice formula is used to calculate the total number stationary
-points one must take pains to eliminate the sign of the determinant
-\cite{Fyodorov_2004_Complexity}. Here we are correct to include it.
+points, one must take pains to eliminate the sign of the determinant
+\cite{Fyodorov_2004_Complexity}. Here it is correct to preserve it.
 
 We need to choose a function $H$ for our calculation. Because $\chi$ is
 a topological invariant, any choice will work so long as it does not share some
-- 
cgit v1.2.3-70-g09d2

