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authorJaron Kent-Dobias <jaron@kent-dobias.com>2020-04-15 14:13:51 -0400
committerJaron Kent-Dobias <jaron@kent-dobias.com>2020-04-15 14:13:51 -0400
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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}