From 75b35bedad9a9b06caedf3083785ac3867b0567c Mon Sep 17 00:00:00 2001
From: Jaron Kent-Dobias <jaron@kent-dobias.com>
Date: Wed, 25 Sep 2019 14:03:19 -0400
Subject: Abstract reword.

---
 main.tex | 15 ++++++++-------
 1 file changed, 8 insertions(+), 7 deletions(-)

(limited to 'main.tex')

diff --git a/main.tex b/main.tex
index 60c7185..a809312 100644
--- a/main.tex
+++ b/main.tex
@@ -57,15 +57,16 @@
 \date\today
 
 \begin{abstract}
-  We develop a phenomenological mean field theory for the elastic response of
-  \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
+  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
   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 a version of the high-pressure
-  antiferromagnetic order modulated along the symmetry axis, and the triple
-  point joining those two phases with the paramagnetic phase is a Lifshitz point.
+  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.
 \end{abstract}
 
 \maketitle
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