From 5aa9d5e00d28c91190a2c07866bb0139275133e3 Mon Sep 17 00:00:00 2001
From: Blaise Thompson <blaise@untzag.com>
Date: Mon, 26 Mar 2018 22:34:02 -0500
Subject: 2018-03-26 22:34

---
 acquisition/chapter.tex | 23 +++++++++++++++--------
 1 file changed, 15 insertions(+), 8 deletions(-)

(limited to 'acquisition')

diff --git a/acquisition/chapter.tex b/acquisition/chapter.tex
index e3035a0..8e75cc1 100644
--- a/acquisition/chapter.tex
+++ b/acquisition/chapter.tex
@@ -1,7 +1,14 @@
-\chapter{Acquistion}
+\chapter{Acquistion} \label{cha:acq}
 
 % TODO: cool quote, if I can think of one
 
+\begin{dquote}
+  The question of software correctness ultimately boils down to, “Does it do what we have in our
+  minds, even the things we have not gotten around to thinking about yet?”
+
+  \dsignature{Alistair Cockburn}
+\end{dquote}
+
 \clearpage
 
 In the Wright Group, \gls{PyCMDS} replaces the old acquisition softwares `ps control', written by
@@ -13,15 +20,15 @@ PyCMDS directly addresses the hardware during experiments.
 
 PyCMDS has, through software improvements alone, dramatically lessened scan times...
 
-\begin{itemize}[topsep=-1.5ex, itemsep=0ex, partopsep=0ex, parsep=0ex, label=$\rightarrow$]
-	\item simultaneous motor motion
+\begin{ditemize}
+  \item simultaneous motor motion
 	\item digital signal processing  % TODO: reference section when it exists
-	\item ideal axis positions \ref{sec:ideal_axis_positions}
-\end{itemize}
+	\item ideal axis positions \ref{acq:sec:ideal_axis_positions}
+\end{ditemize}
 
 \section{Future directions}  % ====================================================================
 
-\subsection{Ideal Axis Positions}\label{sec:ideal_axis_positions}  % ------------------------------
+\subsection{Ideal Axis Positions} \label{acq:sec:ideal_axis_positions}  % -------------------------
 
 Frequency domain multidimensional spectroscopy is a time-intensive process.  %
 A typical \gls{pixel} takes between one-half second and three seconds to acquire.  %
@@ -85,7 +92,7 @@ will also ignore these.  %
 Derivations of the ideal pixel positions for each of these lineshapes appear below.
 % TODO: cite Wright Group quantum beating paper, Kambempati breathing paper
 
-\subsection{Exponential}
+\subsubsection{Exponential}
 
 Simple exponential decays are typically used to describe population and coherence-level dynamics in
 CMDS.  %
@@ -124,7 +131,7 @@ S_n &=& (1-c)\left(\frac{n}{N}\right)^{\frac{\tau_{\mathrm{step}}}{\tau_{\mathrm
 \begin{figure}
 	\includegraphics[scale=0.5]{"processing/PyCMDS/ideal axis positions/exponential"}
 	\caption[TODO]{TODO}
-  \label{fig:exponential_steps}
+  \label{aqn:fig:exponential_steps}
 \end{figure}
 
 \subsubsection{Gaussian}
-- 
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