summaryrefslogtreecommitdiff
diff options
context:
space:
mode:
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
commita3bd2140d76d2ddcadf76812556f02cadb41b493 (patch)
tree30625448200919750c16b672e8dcd31035c1f3b2
parentb07d73fdcc4d1e4c38b473ac10779480a4d678ac (diff)
downloadJPA_55_434006-a3bd2140d76d2ddcadf76812556f02cadb41b493.tar.gz
JPA_55_434006-a3bd2140d76d2ddcadf76812556f02cadb41b493.tar.bz2
JPA_55_434006-a3bd2140d76d2ddcadf76812556f02cadb41b493.zip
New writing in first figure caption.
-rw-r--r--stokes.tex6
1 files changed, 5 insertions, 1 deletions
diff --git a/stokes.tex b/stokes.tex
index 8b89104..095f6cb 100644
--- a/stokes.tex
+++ b/stokes.tex
@@ -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}