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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2020-12-09 11:05:13 +0100 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2020-12-09 11:05:13 +0100 |
commit | 64543b2a1223fb3ed99734415ba87efc2ea95ce9 (patch) | |
tree | 5435a264a840c1302f8d9bb318e6d88dc0837155 | |
parent | 7a3c35fa648374f0f18181cd73588f1febbdcb93 (diff) | |
download | PRR_3_023064-64543b2a1223fb3ed99734415ba87efc2ea95ce9.tar.gz PRR_3_023064-64543b2a1223fb3ed99734415ba87efc2ea95ce9.tar.bz2 PRR_3_023064-64543b2a1223fb3ed99734415ba87efc2ea95ce9.zip |
Updated Jorge's desert figure.
-rw-r--r-- | bezout.tex | 12 | ||||
-rw-r--r-- | fig/desert.pdf | bin | 0 -> 22875 bytes |
2 files changed, 9 insertions, 3 deletions
@@ -329,9 +329,15 @@ is the logarithm of the number of configurations of a given $(a,H_0)$. This problem may be solved exactly with replicas, {\em but it may also be simulated} \cite{Bray_1980_Metastable}. Consider for example the ground-state energy for given $a$, that is, the energy in the limit $\beta_R \rightarrow \infty$ taken adjusting $\beta_I$ so that $\Im H_0=0$ . For $a=1$ this coincides with the ground-state of the real problem. -\begin{center} - \includegraphics[width=6cm]{fig/phase.pdf} -\end{center} +\begin{figure}[htpb] + \centering + \includegraphics{fig/desert.pdf} + \caption{ + The minimum value of $a$ for which the complexity is positive as a function + of (real) energy $\epsilon$ for the pure 4-spin model at several values of + $\kappa$. + } +\end{figure} } \bibliographystyle{apsrev4-2} diff --git a/fig/desert.pdf b/fig/desert.pdf Binary files differnew file mode 100644 index 0000000..a5af1fa --- /dev/null +++ b/fig/desert.pdf |