From 354ce22553f817b6bcabd51502496250396cc4f3 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Wed, 23 Aug 2023 23:40:41 +0200
Subject: No widetext in this context.

---
 when_annealed.tex | 2 --
 1 file changed, 2 deletions(-)

(limited to 'when_annealed.tex')

diff --git a/when_annealed.tex b/when_annealed.tex
index d0323de..60e75c1 100644
--- a/when_annealed.tex
+++ b/when_annealed.tex
@@ -241,7 +241,6 @@ by extremizing an effective action,
   &\quad=\mathop{\mathrm{extremum}}_{q_1,x}\mathcal S_{\oldstylenums1\textsc{rsb}}(q_1,x\mid E,\mu)
 \end{align}
 for the action $\mathcal S_{\oldstylenums1\textsc{rsb}}$ given by \eqref{eq:1rsb.action}.
-\begin{widetext}
   \begin{equation} \label{eq:1rsb.action}
   \begin{aligned}
     &\mathcal S_{\oldstylenums1\textsc{rsb}}(q_1,x\mid E,\mu)
@@ -275,7 +274,6 @@ where $\Delta x=1-x$ and
     -\log\left(\left|\frac{\mu}{\mu_\text m}\right|-\sqrt{\big(\frac\mu{\mu_\text m}\big)^2-1}\right) & \mu^2>\mu_\text m^2
   \end{cases}
 \end{equation}
-\end{widetext}
 The details of the derivation of these expressions can be found in \cite{Kent-Dobias_2023_How}.
 The extremal problem in $\hat\beta$, $r_\mathrm d$, $r_1$, $d_\mathrm d$, and
 $d_1$ has a unique solution and can be found explicitly, but the resulting
-- 
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