From 5e836ed49c669644b9b36eb02d0774b9d6535f60 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Fri, 25 Mar 2022 12:00:10 +0100
Subject: Added new figure.

---
 stokes.tex | 12 ++++++++++++
 1 file changed, 12 insertions(+)

(limited to 'stokes.tex')

diff --git a/stokes.tex b/stokes.tex
index 4b28f39..51b0653 100644
--- a/stokes.tex
+++ b/stokes.tex
@@ -1517,6 +1517,18 @@ constructed by continuing the series for individual thimbles to higher powers
 in $\beta$, which would be equivalent to allowing non-constant terms in the
 Jacobian over the thimble.
 
+\begin{figure}
+  \hfill\includegraphics{figs/obuchi_3-spin.pdf}
+  \caption{
+    Phases of the 3-spin model in the complex-$\beta$, following Obuchi \&
+    Takahashi \cite{Obuchi_2012_Partition-function}. The phase P2 contains a
+    nonzero density of zeros of the partition function, while the `spin-glass'
+    phase SG does not. Analytic continuation via thimbles correctly predicts
+    the boundary between these two phases when $|\beta|\gg1$ to be
+    $\operatorname{Re}\beta=-\epsilon_0$, shown with a dashed line.
+  } \label{fig:obuchi_3-spin}
+\end{figure}
+
 
 \section{The $p$-spin spherical models: numerics}
 
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