From 1537dc5cdc78359399f271b9619d45e9b8c01fe0 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Wed, 15 Apr 2020 14:13:51 -0400
Subject: Nudged the end of widetext.

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

diff --git a/main.tex b/main.tex
index b815c79..15a0268 100644
--- a/main.tex
+++ b/main.tex
@@ -821,6 +821,7 @@ Evaluating at $q=0$, we have
   \end{aligned}
   \label{eq:C0}
 \end{equation}
+\end{widetext}
 Above the transition this has exactly the form of \eqref{eq:static_modulus} for
 any $g$; below the transition it has the same form at $g=0$ to order
 $\eta_*^2$. With $r=a\Delta T+c^2/4D+b^2/C_0$, $u=\tilde u-b^2g/2C_0^2$, and
@@ -831,7 +832,6 @@ $\eta_*^2$. With $r=a\Delta T+c^2/4D+b^2/C_0$, $u=\tilde u-b^2g/2C_0^2$, and
   \end{cases}
 \end{equation}
 we can fit the ratios $b^2/a=1665\,\mathrm{GPa}\,\mathrm K$, $b^2/Dq_*^4=6.28\,\mathrm{GPa}$, and $b\sqrt{-g/\tilde u}=14.58\,\mathrm{GPa}$ with $C_0=(71.14-(0.010426\times T)/\mathrm K)\,\mathrm{GPa}$. The resulting fit the thin solid black line in Fig.~\ref{fig:data}.
-\end{widetext}
 
 \bibliographystyle{apsrev4-1}
 \bibliography{hidden_order}
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