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authorJaron Kent-Dobias <jaron@kent-dobias.com>2022-02-03 10:46:20 +0100
committerJaron Kent-Dobias <jaron@kent-dobias.com>2022-02-03 10:46:20 +0100
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New writing in first figure caption.
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@@ -161,7 +161,11 @@ action potentially has more stationary points. We'll call $\Sigma$ the set of
its complex extension. \textbf{Right:} The stationary points of $\mathcal
S$ in the complex-$\theta$ plane. In this example,
$\Sigma=\{\blacklozenge,\bigstar,\blacktriangle,\blacktriangledown,\bullet,\blacksquare\}$
- and $\Sigma_0=\{\blacklozenge,\blacktriangledown\}$.
+ and $\Sigma_0=\{\blacklozenge,\blacktriangledown\}$. Symmetries exist
+ between the stationary points both as a result of the conjugation symmetry
+ of $\mathcal S$, which produces the vertical reflection, and because in the
+ pure 3-spin models $\mathcal S(-s)=-\mathcal S(s)$, which produces the
+ simultaneous translation and inversion symmetry.
}
\end{figure}