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authorJaron Kent-Dobias <jaron@kent-dobias.com>2018-05-09 18:01:34 -0400
committerJaron Kent-Dobias <jaron@kent-dobias.com>2018-05-09 18:01:34 -0400
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final changes before submissionarxiv_v1
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diff --git a/monte-carlo.tex b/monte-carlo.tex
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@@ -467,12 +467,13 @@ extension to finite field of the behavior at zero field.
\begin{figure}
\centering
\input{fig_correlation_collapse-hL}
- \caption{Collapses of the correlation time $\tau$ of the 2D square lattice
+ \caption{Collapse of the correlation time $\tau$ of the 2D square lattice
Ising model along the critical isotherm at various systems sizes
$N=L\times L$ for $L=8$, $16$, $32$, $64$, $128$, and $256$ as a function
of the renormalization invariant $hL^{\beta\delta/\nu}$. The exponent
$z=0.30$ is taken from recent measurements at zero field
- \cite{liu_dynamic_2014}.
+ \cite{liu_dynamic_2014}. The solid black line shows a plot of
+ $(hL^{\beta\delta/\nu})^{-z\nu/\beta\delta}$.
}
\label{fig:correlation_time-collapse}
\end{figure}