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| -rw-r--r-- | frsb_kac_new.tex | 15 |
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diff --git a/frsb_complexity-2.pdf b/frsb_complexity-2.pdf Binary files differdeleted file mode 100644 index 79c7e64..0000000 --- a/frsb_complexity-2.pdf +++ /dev/null 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} |