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authorJaron Kent-Dobias <jaron@kent-dobias.com>2022-07-11 18:04:40 +0200
committerJaron Kent-Dobias <jaron@kent-dobias.com>2022-07-11 18:04:40 +0200
commit92d6b34550fff868b467511411b22e15482ab397 (patch)
tree73fe32ebfcf11adfd00b65b6ea38e8c22fdc1682
parent1cf4f8a367c55b5fef42f49af5538c7812a92920 (diff)
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More figure work.
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-rw-r--r--figs/24_opt_q(x).pdfbin37694 -> 37694 bytes
-rw-r--r--figs/24_opt_r(x).pdfbin37311 -> 37311 bytes
-rw-r--r--figs/24_opt_xMax.pdfbin41041 -> 41101 bytes
-rw-r--r--figs/24_phases.pdfbin57314 -> 58524 bytes
-rw-r--r--frsb_kac-rice.tex8
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diff --git a/figs/24_opt_d(x).pdf b/figs/24_opt_d(x).pdf
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diff --git a/figs/24_opt_xMax.pdf b/figs/24_opt_xMax.pdf
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diff --git a/frsb_kac-rice.tex b/frsb_kac-rice.tex
index 2e0b971..7a3d798 100644
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+++ b/frsb_kac-rice.tex
@@ -989,19 +989,13 @@ the phase boundary where $q_1$ goes to one.
\includegraphics{figs/316_comparison_b.pdf}
\caption{
- Comparisons between the saddle parameters of the equilibrium solution to
- the $3+16$ model (blue) and those of the complexity (yellow). Equilibrium
- parameters are plotted as functions of the average energy $\langle
- E\rangle=\partial_\beta(\beta F)$ and complexity parameters as functions of
- fixed energy $E$. Solid lines show the result of a 2RSB ansatz, dashed
- lines that of a 1RSB ansatz, and dotted lines that of a RS ansatz. All
- paired parameters coincide at the ground state energy, as expected.
} \label{fig:2rsb.comparison}
\end{figure}
\subsection{Full RSB complexity}
+$\beta_\infty=1$ $\langle E\rangle_\infty=-0.53125$
\begin{figure}
\centering