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@@ -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.