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author | Blaise Thompson <blaise@untzag.com> | 2018-04-09 00:24:18 -0500 |
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committer | Blaise Thompson <blaise@untzag.com> | 2018-04-09 00:24:18 -0500 |
commit | 357568e1fb77afed9dfa203e62da237bf7ce51b3 (patch) | |
tree | 57b8ddafd412934f1e72b7e1f7fe0256480938fd /introduction | |
parent | e43de3cb79a9fad846babf0ddfdca21622b903dc (diff) |
2018-04-09 00:24
Diffstat (limited to 'introduction')
-rw-r--r-- | introduction/chapter.tex | 5 |
1 files changed, 3 insertions, 2 deletions
diff --git a/introduction/chapter.tex b/introduction/chapter.tex index 42943a5..285bd14 100644 --- a/introduction/chapter.tex +++ b/introduction/chapter.tex @@ -28,8 +28,9 @@ dimensionality and selection rules. % With the advent of ultrafast lasers, CMDS can resolve dynamics in excited states and the coupling
between them. \cite{RentzepisPM1970a} %
-CMDS is most often performed in the time domain, where multiple broadband pulses are scanned in
-time to collect a multidimensional interferogram. \cite{MukamelShaul2009a, GallagherSarahM1998a} %
+CMDS is most often performed in the time domain, where multiple broadband pulses are scanned to
+collect a multidimensional interferogram. \cite{MukamelShaul2009a, GallagherSarahM1998a} %
+% BJT: scanned in WHAT? delay? time?
This technique is fast and robust---it has even been performed on a single shot.
\cite{HarelElad2010a} %
However time-domain CMDS has some fundamental limitations:
|