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@@ -462,9 +462,11 @@ ever-closer commensurate values in the style of the devil's staircase \cite{bak_commensurate_1982}. This motivates future \rus\ experiments done at pressure, where the depth of the cusp in the $\Bog$ stiffness should deepen (perhaps with these commensurability jumps) at low pressure and approach zero -like $q_*^4\sim(c_\perp/2D_\perp)^2$ near the Lifshitz point. The presence of -spatial commensurability is not expected to modify the critical behavior -otherwise \cite{garel_commensurability_1976}. +like $q_*^4\sim(c_\perp/2D_\perp)^2$ near the Lifshitz point. Alternatively, +\rus\ done at ambient pressure might examine the heavy fermi liquid to \afm\ +transition by doping. The presence of spatial commensurability is not +expected to modify the critical behavior otherwise +\cite{garel_commensurability_1976}. There are two apparent discrepancies between the orthorhombic strain in the phase diagram presented by \cite{choi_pressure-induced_2018} and that predicted |