From 80baee9f019af151743b3d6e49cddaa44656ac7d Mon Sep 17 00:00:00 2001 From: Blaise Thompson 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. % -- cgit v1.2.3