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@@ -821,6 +821,7 @@ Evaluating at $q=0$, we have \end{aligned} \label{eq:C0} \end{equation} +\end{widetext} Above the transition this has exactly the form of \eqref{eq:static_modulus} for any $g$; below the transition it has the same form at $g=0$ to order $\eta_*^2$. With $r=a\Delta T+c^2/4D+b^2/C_0$, $u=\tilde u-b^2g/2C_0^2$, and @@ -831,7 +832,6 @@ $\eta_*^2$. With $r=a\Delta T+c^2/4D+b^2/C_0$, $u=\tilde u-b^2g/2C_0^2$, and \end{cases} \end{equation} we can fit the ratios $b^2/a=1665\,\mathrm{GPa}\,\mathrm K$, $b^2/Dq_*^4=6.28\,\mathrm{GPa}$, and $b\sqrt{-g/\tilde u}=14.58\,\mathrm{GPa}$ with $C_0=(71.14-(0.010426\times T)/\mathrm K)\,\mathrm{GPa}$. The resulting fit the thin solid black line in Fig.~\ref{fig:data}. -\end{widetext} \bibliographystyle{apsrev4-1} \bibliography{hidden_order} |