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author | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2018-05-09 18:01:34 -0400 |
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committer | Jaron Kent-Dobias <jaron@kent-dobias.com> | 2018-05-09 18:01:34 -0400 |
commit | f18c2b124885a1ba7ed3ebd263da4679c2efed4e (patch) | |
tree | 92bd63216df3cf68e5bc6b20e14fc48e4ddb6481 /monte-carlo.tex | |
parent | 3902c90c737febdd0a501a8762e2ab4e4d1a6513 (diff) | |
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final changes before submissionarxiv_v1
Diffstat (limited to 'monte-carlo.tex')
-rw-r--r-- | monte-carlo.tex | 5 |
1 files changed, 3 insertions, 2 deletions
diff --git a/monte-carlo.tex b/monte-carlo.tex index 8eef5b0..f88a053 100644 --- a/monte-carlo.tex +++ b/monte-carlo.tex @@ -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} |