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@@ -118,13 +118,14 @@ theories~\cite{kambe_odd-parity_2018, haule_arrested_2009,
rau_hidden_2012, riggs_evidence_2015, hoshino_resolution_2013,
ikeda_theory_1998, chandra_hastatic_2013, harrison_hidden_nodate,
ikeda_emergent_2012} propose associating any of a variety of broken symmetries
-with \ho. This work analyzes a phenomenological model with order parameters of
-general symmetry that couple linearly to strain. Of these, only one is compatible
-with two experimental observations: first, the $\Bog$ ``nematic" elastic
-susceptibility $(C_{11}-C_{12})/2$ softens anomalously from room temperature
-down to $T_{\text{\ho}}=17.5\,\K$;\cite{de_visser_thermal_1986} and second, a
-$\Bog$ nematic distortion is observed by x-ray scattering under sufficient
-pressure to destroy the \ho\ state.\cite{choi_pressure-induced_2018}
+with \ho. This work analyzes a family of phenomenological models with order
+parameters of general symmetry that couple linearly to strain. Of these, only
+one is compatible with two experimental observations: first, the $\Bog$
+``nematic" elastic susceptibility $(C_{11}-C_{12})/2$ softens anomalously from
+room temperature down to
+$T_{\text{\ho}}=17.5\,\K$;\cite{de_visser_thermal_1986} and second, a $\Bog$
+nematic distortion is observed by x-ray scattering under sufficient pressure to
+destroy the \ho\ state.\cite{choi_pressure-induced_2018}
Recent resonant ultrasound spectroscopy (\rus) measurements were used to
examine the thermodynamic discontinuities in the elastic moduli at