Update on Overleaf.

1 files changed, 3 insertions, 5 deletions

diff --git a/main.tex b/main.tex
index 8af828b..2c6682b 100644
--- a/main.tex
+++ b/main.tex
@@ -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 of order parameters of
-general symmetry, linearly coupled to strain. We identify yet another mechanism
+general symmetry that couple linearly to strain. We identify yet another mechanism
 that is best compatible with two experimental observations: first, the $\Bog$
 ``nematic" elastic susceptibility $(C_{11}-C_{12})/2$ softens anomalously from
 room temperature down to
@@ -547,10 +547,8 @@ 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