From f18c2b124885a1ba7ed3ebd263da4679c2efed4e Mon Sep 17 00:00:00 2001 From: Jaron Kent-Dobias Date: Wed, 9 May 2018 18:01:34 -0400 Subject: final changes before submission --- monte-carlo.tex | 5 +++-- 1 file changed, 3 insertions(+), 2 deletions(-) (limited to 'monte-carlo.tex') 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} -- cgit v1.2.3-54-g00ecf