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authorJaron Kent-Dobias <jaron@kent-dobias.com>2022-07-12 16:29:09 +0200
committerJaron Kent-Dobias <jaron@kent-dobias.com>2022-07-12 16:29:09 +0200
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Cleaned up Jorge's addition.
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diff --git a/frsb_kac-rice.tex b/frsb_kac-rice.tex
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@@ -404,18 +404,19 @@ where the function $\mathcal D$ is defined by
\end{aligned}
\end{equation}
-{\color{blue}
By fixing the trace of the Hessian, we have effectively fixed
-the value of the stability $\mu$ in all replicas to the value $\mu^*$.\\
+the value of the stability $\mu$ in all replicas to the value $\mu^*$.
+\begin{itemize}
+ \item For $\mu^*<\mu_m$, this amounts to fixing the index density. Since the
+ overwhelming majority of saddles have a semicircle distribution, the
+ fluctuations are rarer than exponential.
+ \item For the gapped case $\mu^*>\mu_m$, there is a an exponentially small
+ probability that $r=1,2,...$ eigenvalues detach from the semicircle in such
+ a way that the index is in fact $N {\cal{I}}=r$. We shall not discuss
+ these subextensive index fluctuations in this paper, the interested reader
+ may find what is needed in \cite{Auffinger_2013_Complexity}.
+\end{itemize}
-$\bullet$ For $\mu^*<\mu_m$, this amounts to fixing the index density. The argument is that
-the overwhelming majority of saddles have a semicircle distribution, the fluctuations are rarer than exponential.
-
-$\bullet$ For the gapped case $\mu^*>\mu_m$, there is a an exponentially small probability that $r=1,2,...$ eigenvalues detach
-from the semicircle in such a way that the index is in fact $N {\cal{I}}=r$.
-We shall not discuss these index fluctuations in this paper, the interested
-reader may find what is needed in \cite{Auffinger_2013_Complexity}
-}
\subsubsection{The gradient factors}
The $\delta$-functions in the remaining factor are treated by writing them in