From 568269ca29871b02b918f5c8a3d142888b887903 Mon Sep 17 00:00:00 2001
From: Blaise Thompson <blaise@untzag.com>
Date: Thu, 10 May 2018 11:08:59 -0500
Subject: 2018-05-10 11:08

---
 MX2/chapter.tex | 27 +++------------------------
 1 file changed, 3 insertions(+), 24 deletions(-)

(limited to 'MX2/chapter.tex')

diff --git a/MX2/chapter.tex b/MX2/chapter.tex
index 98c37cc..6cfcdf8 100644
--- a/MX2/chapter.tex
+++ b/MX2/chapter.tex
@@ -391,7 +391,7 @@ the square root of the measured FWM signal since FWM depends quadratically on th
 concentration and path length.  %
 
 The main set of data presented in this work is an $\omega_1\omega_2\tau_{21}$ ``movie'' with
-$\tau_{22\prime}=0$. 
+$\tau_{22\prime}=0$.
 \autoref{fig:Czech03} shows representative 2D frequency-frequency slices from this movie at
 increasingly negative $\tau_{21}$ times.  %
 Each 2D frequency spectrum contains side plots along both axes that compare the absorbance spectrum
@@ -477,8 +477,8 @@ features when $\omega_1=\omega_2$ or the cross-peak features when $\omega_1\neq\
 The stimulated emission (SE) and ground-state bleaching (GSB) pathways create the eg or e$^\prime$g
 output coherences from the ee and gg populations, respectively, while the excited-state absorption
 pathway creates the 2e,e or e$^\prime$+e,e biexcitonic output coherences.  %
-\autoref{fig:Czech06} also includes a population transfer pathway from the ee excited-state
-population to an e$^\prime$e$^\prime$ population from which similar SE and ESA pathways occur.  %
+There is also a population transfer pathway from the ee excited-state population to an
+e$^\prime$e$^\prime$ population from which similar SE and ESA pathways occur.  %
 Since the ESA pathways destructively interfere with the SE and GSB pathways, the output singal
 depends on the differences between the pathways.  %
 Factors that change the biexcitonic output coherences such as the transition moments, state filling
@@ -501,18 +501,6 @@ A quantitative treatment of the cancellation effects between the GSB, SE, and ES
 knowledge of the transition moments and state degeneracies and is beyond the scope of this paper.
 \cite{WongCathyY2011a}  %
 
-\begin{figure}
-  \includegraphics[width=0.5\textwidth]{MX2/06}
-  \caption[Liouville pathways in time orderings V, VI.]{
-    Liouville pathways for \autoref{fig:Czech04}. gg and
-    ee designate ground- and excited-state populations, the eg, 2e,e, and e$^\prime$+e,e represent
-    the excitonic and biexcitonic output coherences, and the arrows are labeled with the
-    frequencies or population transfer responsible for the transitions. e and e$^\prime$ represent
-    either A or B excitonic states.
-  }
-  \label{fig:Czech06}
-\end{figure}
-
 The most important characteristic of the experimental spectra is the contrast between the absence
 of well-resolved excitonic features that depend on $\omega_2$ in Figures \ref{fig:Czech03} and
 \ref{fig:Czech05} and the well-defined excitonic features that depend on $\omega_1$.  %
@@ -632,15 +620,6 @@ increasingly positive delays.  %
   \label{fig:Czech08}
 \end{figure}
 
-\begin{figure}
-  \includegraphics[width=0.5\textwidth]{MX2/09}
-  \caption[Liouville pathways in time orderings I, III.]{
-    Liouville pathways for the $\omega_1$, $\omega_2$,
-    and $\omega_{2^\prime}$ time ordering of pulse interactions. e and e$^\prime$ represent either
-    A or B excitonic states.}
-  \label{fig:Czech09}
-\end{figure}
-
 \section{Conclusions}  % ==========================================================================
 
 This paper presents the first coherent multidimensional spectroscopy of MoS\textsubscript{2} thin
-- 
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