more figure tweaks

1 files changed, 1 insertions, 1 deletions

diff --git a/main.tex b/main.tex
index 53a4833..f4f2b71 100644
--- a/main.tex
+++ b/main.tex
@@ -439,7 +439,7 @@ where $\eta$ has a large nonzero value and higher powers in the free energy
 become important. The data in the high-temperature phase can be fit to the
 theory \eqref{eq:elastic.susceptibility}, with a linear background modulus
 $C^0_\Bog$ and $\tilde r-\tilde r_c=a(T-T_c)$, and the result is shown in
-Figure \ref{fig:fit}. The data and theory appear quantitatively consistent in
+Figure \ref{fig:data}. The data and theory appear quantitatively consistent in
 the high temperature phase, suggesting that \ho\ can be described as a
 $\Bog$-nematic phase that is modulated at finite $q$ along the $c-$axis.