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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-02-03 10:46:20 +0100 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2022-02-03 10:46:20 +0100 |
commit | a3bd2140d76d2ddcadf76812556f02cadb41b493 (patch) | |
tree | 30625448200919750c16b672e8dcd31035c1f3b2 | |
parent | b07d73fdcc4d1e4c38b473ac10779480a4d678ac (diff) | |
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New writing in first figure caption.
-rw-r--r-- | stokes.tex | 6 |
1 files changed, 5 insertions, 1 deletions
@@ -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} |