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@@ -204,6 +204,8 @@ coupling to linear order is
\begin{equation}
f_\i=-b^{(i)}\epsilon_\X^{(i)}\eta.
\end{equation}
+Many high-order interations are permitted, and in the appendix another of the
+form $\epsilon^2\eta^2$ is added to the following analysis.
If there exists no component of strain that transforms like the representation
$\X$ then there can be no linear coupling. The next-order coupling is linear in
strain, quadratic in order parameter, and the effect of this coupling at a