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@@ -546,7 +546,7 @@ This motivates future ultrasound experiments done under pressure, where the depth of the cusp in the $\Bog$ modulus should deepen (perhaps with these commensurability jumps) at low pressure and approach zero as $q_*^4\sim(c_\perp/2D_\perp)^2$ near the Lifshitz point. -Alternatively, \rus\ done at ambient pressure might examine the heavy fermi +Alternatively, \rus\ done at ambient pressure might examine the heavy Fermi liquid to \afm\ transition by doping. Though previous \rus\ studies have doped \urusi\ with Rhodium,\cite{yanagisawa_ultrasonic_2014} the magnetic nature of Rhodium ions likely artificially promotes magnetic phases. A dopant like @@ -605,12 +605,12 @@ in the associated elastic modulus. In this picture, the \ho\ phase is characterized by uniaxial modulated $\Bog$ order, while the high pressure phase is characterized by uniform $\Bog$ order. -The coinciding of our theory's orthorhombic high-pressure phase and \urusi's +The coincidence of our theory's orthorhombic high-pressure phase and \urusi's \afm\ is compelling, but our mean field theory does not make any explicit -connection with the physics of \afm. This may be reasonable since correlations -often lead to \afm\ as a secondary effect, like in many Mott insulators. An +connection with the physics of \afm. Neglecting this physics could be reasonable since correlations +often lead to \afm\ as a secondary effect, like what occurs in many Mott insulators. An electronic theory of this phase diagram may find that the \afm\ observed in -\urusi\ indeed follows along with a high-pressure orthorhombic phase associated with +\urusi\ indeed follows along with an independent high-pressure orthorhombic phase associated with uniform $\Bog$ electronic order. The corresponding prediction of uniform $\Bog$ symmetry breaking in the high |