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-rw-r--r--when_annealed.tex2
1 files changed, 0 insertions, 2 deletions
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