From f18c2b124885a1ba7ed3ebd263da4679c2efed4e Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
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

