From 357568e1fb77afed9dfa203e62da237bf7ce51b3 Mon Sep 17 00:00:00 2001 From: Blaise Thompson 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 -- cgit v1.2.3