1 files changed, 7 insertions, 7 deletions
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.  %