From 7b507a18e841f56a534dad25e1a68a17cf6fe280 Mon Sep 17 00:00:00 2001 From: Blaise Thompson Date: Wed, 28 Feb 2018 19:47:36 -0600 Subject: 2018-02-28 19:47 --- mixed_domain/chapter.tex | 14 +++++++------- 1 file changed, 7 insertions(+), 7 deletions(-) (limited to 'mixed_domain') diff --git a/mixed_domain/chapter.tex b/mixed_domain/chapter.tex index aad2be1..12b0278 100644 --- a/mixed_domain/chapter.tex +++ b/mixed_domain/chapter.tex @@ -85,7 +85,7 @@ shift (3PEPS) \cite{EmdeMichelF1998a, DeBoeijWimP1996a, DeBoeijWimP1995a, ChoMin These methods also include fully-coherent methods involving only coherences such as Stimulated Raman Spectroscopy (SRS) \cite{YoonSangwoon2005a, McCamantDavidW2005a}, Doubly Vibrationally Enhanced (DOVE) \cite{ZhaoWei1999a, ZhaoWei1999b, ZhaoWei2000a, MeyerKentA2003a, - DonaldsonPaulM2007a, DonaldsonPaulM2008a, FournierFrederic2008a}, + 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, @@ -106,13 +106,13 @@ capabilities for measuring homogeneous and inhomogeneous broadening. % Although these experiments are typically described in the driven limit, \cite{GallagherSarahM1998a, FourkasJohnT1992a, FourkasJohnT1992b} many of the experiments involve pulse widths that are comparable to the widths of the system. \cite{MeyerKentA2003a, - DonaldsonPaulM2007a, PakoulevAndreiV2009a, ZhaoWei1999a, CzechKyleJonathan2015a, + DonaldsonPaulMurray2007b, PakoulevAndreiV2009a, ZhaoWei1999a, CzechKyleJonathan2015a, KohlerDanielDavid2014a} % MR-CMDS then becomes a mixed-domain experiment whereby resonances are characterized with marginal resolution in both frequency and time. % For example, DOVE spectroscopy involves three different pathways \cite{WrightJohnCurtis2003a} whose relative importance depends on the relative importance of FID and driven -responses. \cite{DonaldsonPaulM2010a} % +responses. \cite{DonaldsonPaulMurray2010a} % In the driven limit, the DOVE line shape depends on the difference between the first two pulse frequencies so the line shape has a diagonal character that mimics the effects of inhomogeneous broadening. % @@ -679,8 +679,8 @@ amplitudes at $t=0$ (driven) and at $t / \Delta_t=2$ (FID); amplitudes for all $\Omega_{fx}/\Delta_{\omega}$ values shown are comparable at $t=0$, but the lack of FID formation for $\Omega_{fx}/\Delta_{\omega}=\pm2$ manifests as a visibly disproportionate amplitude decay. % Many ultrafast spectroscopies take advantage of the latent FID to suppress non-resonant background, -improving signal to noise. \cite{LagutchevAlexi2007a, LagutchevAlexi2010a, DonaldsonPaulM2010a, - DonaldsonPaulM2008a} % +improving signal to noise. \cite{LagutchevAlexi2007a, LagutchevAlexi2010a, + DonaldsonPaulMurray2010a, DonaldsonPaulMurray2008a} % In driven experiments, the output frequency and line shape are fully constrained by the excitation beams. % @@ -863,8 +863,8 @@ As a result, the line shape acquires a diagonal character. % The changes in line shape seen in Fig. \ref{fig:pw1} have significant ramifications for the interpretations and strategies of MR-CMDS in the mixed domain. % Time-gating has been used to isolate the 2D spectra of a certain -time-ordering\cite{MeyerKentA2004a, PakoulevAndreiV2006a, DonaldsonPaulM2007a}, but here we show that -time-gating itself causes significant line shape changes to the isolated pathways. % +time-ordering\cite{MeyerKentA2004a, PakoulevAndreiV2006a, DonaldsonPaulMurray2007b}, but here we +show that time-gating itself causes significant line shape changes to the isolated pathways. % The phenomenon of time-gating can cause frequency and delay axes to become functional of each other in unexpected ways. % -- cgit v1.2.3