From 357568e1fb77afed9dfa203e62da237bf7ce51b3 Mon Sep 17 00:00:00 2001
From: Blaise Thompson <blaise@untzag.com>
Date: Mon, 9 Apr 2018 00:24:18 -0500
Subject: 2018-04-09 00:24

---
 abstract.tex | 4 +++-
 1 file changed, 3 insertions(+), 1 deletion(-)

(limited to 'abstract.tex')

diff --git a/abstract.tex b/abstract.tex
index 64d230f..5ef1404 100644
--- a/abstract.tex
+++ b/abstract.tex
@@ -24,6 +24,7 @@ The pulses interact with the material, and due to the specific interference betw
 fields the material is driven to emit a new pulse: the MR-CMDS signal.  %
 This signal may be different in frequency from the input pulses, and it may travel in a new
 direction depending on the exact experiment being performed.  %
+% BJT: flip proceeding sentence around
 The MR-CMDS experiment involves tracking the intensity of this output signal as a function of
 different properties of the excitation pulses.  %
 These properties include
@@ -33,10 +34,11 @@ These properties include
 4. polarization \cite{FournierFrederic2009a}, among others.  %
 Thus MR-CMDS can be thought of as a multidimensional experimental space, where experiments
 typically involve explorations in one to four of the properties above.  %
+% BJT: emphasize UP TO four dimensions, practically
 
 Because MR-CMDS is a family of related-but-separate experiments, each of them a multidimensional
 space, there are special challenges that must be addressed when designing a general-purpose MR-CMDS
-instrument.  %
+instrument.  % BJT: be more specific about the challenge at hand
 These issues require development of software, hardware, and theory.  %
 Five different improvements to MR-CMDS are presented in this dissertation: 1. processing software
 (\autoref{cha:pro}), 2. acquisition software (\autoref{cha:acq}) 3, active artifact correction
-- 
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