From 6579cbe6381ee4bb805a6d5b5cc5fbd249daa9f2 Mon Sep 17 00:00:00 2001 From: Blaise Thompson Date: Mon, 16 Apr 2018 09:35:25 -0500 Subject: 2018-04-16 09:35 --- mixed_domain/chapter.tex | 6 +++--- 1 file changed, 3 insertions(+), 3 deletions(-) (limited to 'mixed_domain/chapter.tex') diff --git a/mixed_domain/chapter.tex b/mixed_domain/chapter.tex index 0880ecc..60910c2 100644 --- a/mixed_domain/chapter.tex +++ b/mixed_domain/chapter.tex @@ -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 -- cgit v1.2.3