Draft edits to Figure caption to reflect new theory lines.

1 files changed, 4 insertions, 7 deletions

diff --git a/main.tex b/main.tex
index 15a0268..3da57a9 100644
--- a/main.tex
+++ b/main.tex
@@ -472,22 +472,19 @@ corresponding modulus.
   \caption{
     \Rus\ measurements of the elastic moduli of \urusi\ at ambient pressure as a
     function of temperature from recent experiments\cite{1903.00552v1} (blue,
-    solid) alongside fits to theory (magenta, dashed). The solid yellow region
+    solid) alongside fits to theory (magenta, dashed and black, solid). The solid yellow region
     shows the location of the \ho\ phase. (a) $\Btg$ modulus data and a fit to
     the standard form.\cite{Varshni_1970} (b) $\Bog$ modulus data and a fit to
-    \eqref{eq:static_modulus}. The fit gives
+    \eqref{eq:static_modulus} (magenta, dashed) and a fit to \eqref{eq:C0} (black, solid). The fit gives
     $C^0_\Bog\simeq\big[71-(0.010\,\K^{-1})T\big]\,\GPa$, $D_\perp
     q_*^4/b^2\simeq0.16\,\GPa^{-1}$, and
     $a/b^2\simeq6.1\times10^{-4}\,\GPa^{-1}\,\K^{-1}$. Addition of a quadratic
     term in $C^0_\Bog$ was here not needed for the fit.\cite{Varshni_1970} (c)
     $\Bog$ modulus data and the fit of the \emph{bare} $\Bog$ modulus. (d)
-    $\Bog$ modulus data and the fit transformed by
+    $\Bog$ modulus data and the fits transformed by
     $[C^0_\Bog(C^0_\Bog/C_\Bog-1)]]^{-1}$, which is predicted from
     \eqref{eq:static_modulus} to equal $D_\perp q_*^4/b^2+a/b^2|T-T_c|$, e.g.,
-    an absolute value function. The failure of the Ginzburg--Landau prediction
-    below the transition is expected on the grounds that the \op\ is too large
-    for the free energy expansion to be valid by the time the Ginzburg
-    temperature is reached.
+    an absolute value function.
   }
   \label{fig:data}
 \end{figure*}