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author | Blaise Thompson <blaise@untzag.com> | 2018-04-07 18:20:04 -0500 |
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committer | Blaise Thompson <blaise@untzag.com> | 2018-04-07 18:20:04 -0500 |
commit | 80baee9f019af151743b3d6e49cddaa44656ac7d (patch) | |
tree | 0ed7337ae271f4a5b2d2af1e356cb205ad870a04 /spectroscopy | |
parent | 97c0cce9063212e416ece9c6fef95b33841800c5 (diff) |
2018-04-07 18:20
Diffstat (limited to 'spectroscopy')
-rw-r--r-- | spectroscopy/chapter.tex | 9 |
1 files changed, 2 insertions, 7 deletions
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. %
|