From 80baee9f019af151743b3d6e49cddaa44656ac7d Mon Sep 17 00:00:00 2001
From: Blaise Thompson <blaise@untzag.com>
Date: Sat, 7 Apr 2018 18:20:04 -0500
Subject: 2018-04-07 18:20

---
 spectroscopy/chapter.tex | 9 ++-------
 1 file changed, 2 insertions(+), 7 deletions(-)

(limited to 'spectroscopy/chapter.tex')

diff --git a/spectroscopy/chapter.tex b/spectroscopy/chapter.tex
index a70cd69..b07a407 100644
--- a/spectroscopy/chapter.tex
+++ b/spectroscopy/chapter.tex
@@ -232,14 +232,9 @@ pulse, and pulses with very large frequency bandwidth (very short in time) becom
 and control.   %
 With short, broad pulses:
 \begin{ditemize}
-	\item Non-resonant signal becomes brighter relative to resonant signal. [CITE]
-	\item Pulse distortions become important. [CITE JONAS]
+	\item Non-resonant signal becomes brighter relative to resonant signal. \cite{ChengJixin2001a}
+	\item Pulse distortions become essentially unavoidable. \cite{SpencerAustinP2015a}
 \end{ditemize}
-%This epi-CARS paper might have some useful discussion of non-resonant vs resonant for shorter and
-%shorter pulses \cite{ChengJixin2001a}.  %
-%An excellent discussion of pulse distortion phenomena in broadband time-domain experiments was
-%published by \textcite{SpencerAustinP2015a}.  %
-%See Paul's dissertation
 
 Time domain experiments require a phase-locked, independently controlled local oscillator in order
 to collect the interferogram at the heart of such techniques.  %
-- 
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