From f4d037b88c9ccabbe462b84a6ebb13d1e74e6094 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Fri, 10 Jun 2022 21:27:41 +0200
Subject: Updated figure.

---
 frsb_complexity-2.pdf | Bin 11953 -> 0 bytes
 frsb_kac_new.tex      |  15 ++++++++++-----
 2 files changed, 10 insertions(+), 5 deletions(-)
 delete mode 100644 frsb_complexity-2.pdf

diff --git a/frsb_complexity-2.pdf b/frsb_complexity-2.pdf
deleted file mode 100644
index 79c7e64..0000000
Binary files a/frsb_complexity-2.pdf and /dev/null differ
diff --git a/frsb_kac_new.tex b/frsb_kac_new.tex
index 1efb9ba..e8b57c8 100644
--- a/frsb_kac_new.tex
+++ b/frsb_kac_new.tex
@@ -456,11 +456,16 @@ When minima dominate, $\mu>\mu_m$ and all the roots inside $\mathcal D(\mu)$ are
 \end{equation}
 
 \begin{figure}
-\begin{center}
-\includegraphics[width=13cm]{frsb_complexity-2.pdf}
-\end{center}
-\caption{
-} \label{fig:frsb.complexity}
+  \centering
+  \includegraphics{figs/24_complexity.pdf}
+  \caption{
+    The complexity $\Sigma$ of the mixed $2+4$ spin model as a function of
+    distance $\Delta\epsilon=\epsilon-\epsilon_0$ of the ground state. The
+    solid blue line shows the complexity of dominant saddles given by the FRSB
+    ansatz, and the solid yellow line shows the complexity of marginal minima.
+    The dashed lines show the same for the annealed complexity. The inset shows
+    more detail around the ground state.
+  } \label{fig:frsb.complexity}
 \end{figure}
 
 \subsubsection{Recovering the replica ground state}
-- 
cgit v1.2.3-70-g09d2