From e0115f4fcad6794b09c96b2dee843d73e5c14080 Mon Sep 17 00:00:00 2001
From: bradramshaw undefined <bradramshaw@cornell.edu>
Date: Mon, 7 Oct 2019 02:14:14 +0000
Subject: Update on Overleaf.

---
 main.tex | 10 ++++------
 1 file changed, 4 insertions(+), 6 deletions(-)

(limited to 'main.tex')

diff --git a/main.tex b/main.tex
index 84ca09c..ea68802 100644
--- a/main.tex
+++ b/main.tex
@@ -4,6 +4,8 @@
 \usepackage{amsmath,graphicx,upgreek,amssymb,xcolor}
 \usepackage[colorlinks=true,urlcolor=purple,citecolor=purple,filecolor=purple,linkcolor=purple]{hyperref}
 
+\newcommand{\brad}[1]{{\color{red} #1}}
+
 % Our mysterious boy
 \def\urusi{URu$_{\text2}$Si$_{\text2}$}
 
@@ -60,14 +62,10 @@
 \begin{abstract}
   We develop a phenomenological mean field theory for the strain in \urusi\
   through its hidden order transition. Several experimental features are
-  reproduced when the order parameter has $\Bog$ symmetry: the topology of the
-  temperature--pressure phase diagram, the response of the strain stiffness
+  reproduced when the order parameter is of the $\Bog$ representation: the topology of the temperature--pressure phase diagram, the response of the strain stiffness
   tensor above the hidden-order transition at zero pressure, and orthorhombic
   symmetry breaking in the high-pressure antiferromagnetic phase. In this
-  scenario, the hidden order is characterized by the order parameter in the
-  high-pressure antiferromagnetic phase modulated along the symmetry axis, and
-  the triple point joining those two phases with the paramagnetic phase is a
-  Lifshitz point.
+  scenario, hidden order is characterized by broken rotational symmetry that is modulated along the symmetry axis, the primary order of the high-pressure phase is an unmodulated nematic state, and the triple point joining those two phases with the paramagnetic phase is a Lifshitz point.
 \end{abstract}
 
 \maketitle
-- 
cgit v1.2.3-70-g09d2

