From ac27d79183ce80993bc332d6e09e0e12cb967fc3 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Sat, 7 Oct 2023 15:29:08 +0200
Subject: Some work.

---
 marginal.tex | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

(limited to 'marginal.tex')

diff --git a/marginal.tex b/marginal.tex
index 96c2a99..b840699 100644
--- a/marginal.tex
+++ b/marginal.tex
@@ -141,7 +141,7 @@ we expect no $b$-dependence of this matrix. $A^{aa}$ is the usual
 replica-symmetric overlap matrix of the spherical two-spin problem. $A^{ab}$
 describes overlaps between eigenvectors at different stationary points and should be a constant $m_a\times m_b$ matrix.
 
-We will discuss at the end of this paper when these order parameters can be expected to be nonzero, but in this problem all of the $X$s, $\hat X$s, and $A^{ab}$ for $a\neq b$ are zero.
+We will discuss at the end of this paper when these order parameters can be expected to be nonzero, but in this and most isotropic problems all of the $X$s, $\hat X$s, and $A^{ab}$ for $a\neq b$ are zero.
 
 \begin{equation}
   \begin{aligned}
-- 
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