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authorBlaise Thompson <blaise@untzag.com>2018-04-16 09:35:25 -0500
committerBlaise Thompson <blaise@untzag.com>2018-04-16 09:35:25 -0500
commit6579cbe6381ee4bb805a6d5b5cc5fbd249daa9f2 (patch)
tree3f4694c6bd0a21ea1321c18ed8ab535ddf07e5fb /mixed_domain
parent3671f4e2c92f28319e9c8e44071604e98d8d783f (diff)
2018-04-16 09:35
Diffstat (limited to 'mixed_domain')
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@@ -88,8 +88,8 @@ Enhanced (DOVE) \cite{ZhaoWei1999a, ZhaoWei1999b, ZhaoWei2000a, MeyerKentA2003a,
DonaldsonPaulMurray2007b, DonaldsonPaulMurray2008a, FournierFrederic2008a},
Triply Resonant Sum Frequency (TRSF) \cite{BoyleErinSelene2013a, BoyleErinSelene2013b,
BoyleErinSelene2014a}, Sum Frequency Generation (SFG) \cite{LagutchevAlexi2007a}, Coherent
-Anti-Stokes Raman Spectroscopy (CARS) \cite{CarlsonRogerJ1990b, CarlsonRogerJ1990c,
- CarlsonRogerJ1991a}, and other coherent Raman methods \cite{SteehlerJK1985a}. %
+Anti-Stokes Raman Spectroscopy (CARS) \cite{CarlsonRogerJohn1990b, CarlsonRogerJohn1990c,
+ CarlsonRogerJohn1991a}, and other coherent Raman methods \cite{SteehlerJK1985a}. %
This paper focuses on understanding the nature of the spectral changes that occur in Coherent
Multidimensional Spectroscopy (CMDS) as experiments transition between the two limits of frequency-
@@ -346,7 +346,7 @@ from the pulse delay times represented in \autoref{mix:fig:overview}b. %
\subsection{Inhomogeneity} % ---------------------------------------------------------------------
Inhomogeneity is isolated in CMDS through both spectral signatures, such as
-line-narrowing \cite{BesemannDanielM2004a, OudarJL1980a, CarlsonRogerJ1990a, RiebeMichaelT1988a,
+line-narrowing \cite{BesemannDanielM2004a, OudarJL1980a, CarlsonRogerJohn1990a, RiebeMichaelT1988a,
SteehlerJK1985a}, and temporal signatures, such as photon echoes \cite{WeinerAM1985a,
AgarwalRitesh2002a}. %
We simulate the effects of static inhomogeneous broadening by convolving the homogeneous response