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authorJaron Kent-Dobias <jaron@kent-dobias.com>2019-12-18 17:12:43 -0500
committerJaron Kent-Dobias <jaron@kent-dobias.com>2019-12-18 17:12:43 -0500
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@@ -119,7 +119,7 @@ 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, linearly coupled to strain. Of these, only one is compatible
+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
@@ -546,10 +546,8 @@ pressure, where the depth of the cusp in the $\Bog$ modulus should deepen
as $q_*^4\sim(c_\perp/2D_\perp)^2$ near the Lifshitz point.
Alternatively, \rus\ done at ambient pressure might examine the heavy Fermi
liquid to \afm\ transition by doping. 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
-phosphorous that only exerts chemical pressure might more faithfully explore
-the pressure axis of the phase diagram. Our work also motivates experiments
+\urusi\ with Rhodium,\cite{yanagisawa_ultrasonic_2014} the magnetic rhodium dopants likely promote magnetic phases. A non-magnetic dopant such as phosphorous may more faithfully explore
+the transition out of the HO phase. Our work also motivates experiments
that can probe the entire correlation function---like x-ray and neutron
scattering---and directly resolve its finite-$q$ divergence. The presence of
spatial commensurability is known to be irrelevant to critical behavior at a