From bc455f449cab2c1c36baf257bdafc48653947091 Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Thu, 27 Feb 2020 20:53:15 -0500
Subject: small changes for brad

---
 poster_aps_mm_2020.tex | 14 +++++++-------
 1 file changed, 7 insertions(+), 7 deletions(-)

diff --git a/poster_aps_mm_2020.tex b/poster_aps_mm_2020.tex
index 90e3794..b156dbe 100644
--- a/poster_aps_mm_2020.tex
+++ b/poster_aps_mm_2020.tex
@@ -4,7 +4,7 @@
 \usepackage[utf8]{inputenc}
 \usepackage[T1]{fontenc}
 \usepackage[]{amsmath}
-\usepackage{amssymb,latexsym,mathtools,multicol,lipsum,wrapfig,floatrow}
+\usepackage{amssymb,latexsym,mathtools,multicol,lipsum,wrapfig,floatrow,bm}
 \usepackage[font=normalsize,labelfont=bf]{caption}
 \usepackage{tgheros}
 \usepackage[helvet]{sfmath}
@@ -96,7 +96,7 @@
 
   \hspace{1em}
   The modulus tensor of \urusi\ anomalously softens over several hundred
-  Kelvin and is cut off by the \ho\ transition.
+  Kelvin and is cut off by the \ho\ transition, seen in Fig.~\ref{fig:plots}(b).
   \textbf{
     We show that only one order parameter symmetry is consistent with this
     softening and the topology of the phase diagram.
@@ -108,7 +108,7 @@
 
   \hspace{1em}
   Resonant ultrasound spectroscopy drives a sample with sound and measures its
-  resonances by looking for spikes in the response. Using the sample geometry
+  resonances by looking for peaks in the response. Using the sample geometry
   and the location of sufficiently many resonances, the modulus tensor
   $C$---which gives the energetic cost of strain---can be calculated.
   \textbf{
@@ -149,7 +149,7 @@
 
 
 
-  \section{Landau--Ginzburg theory}
+  \section{Landau theory}
   \Large
 
   \hspace{1em}
@@ -158,8 +158,8 @@
   only if they correspond to the same irrep. Higher order couplings lead to
   thermodynamic discontinuities but not diverging responses.
   \textbf{
-    The anomalous softening of \urusi\ suggests the hidden order parameter
-    couples linearly to strain.
+    The anomalous softening of \urusi\ in Fig.~\ref{fig:plots}(b) suggests the
+    hidden order parameter couples linearly to strain.
   }
 
   \hspace{1em}
@@ -202,7 +202,7 @@
 
   \hspace{1em}
   \textbf{
-    This theory has a \emph{Lifshitz triple point} at $\tilde r=c_\perp=0$.
+    This theory has a \emph{Lifshitz triple point} at $\bm{\tilde r=c_\perp=0}$.
   }
   The three phases that meet are
   \begin{itemize}
-- 
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