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-rw-r--r--PEDOT:PSS/chapter.tex40
1 files changed, 20 insertions, 20 deletions
diff --git a/PEDOT:PSS/chapter.tex b/PEDOT:PSS/chapter.tex
index 8bb1510..1e26434 100644
--- a/PEDOT:PSS/chapter.tex
+++ b/PEDOT:PSS/chapter.tex
@@ -71,7 +71,7 @@ processing. %
thin film used in this work. %
\clearpage
-\begin{dfigure}
+\begin{figure}
\centering
\includegraphics[width=0.5\linewidth]{"PEDOT:PSS/linear"}
\caption[PEDOT:PSS transmission and reflectance spectra.]{
@@ -80,7 +80,7 @@ thin film used in this work. %
Extinction is $\log_{10}{\mathsf{(transmission)}}$. %
}
\label{fig:PEDOTPSS_linear}
-\end{dfigure}
+\end{figure}
\clearpage
\section{Three-pulse echo spectroscopy} % --------------------------------------------------------
@@ -98,7 +98,7 @@ that all three excitation pulse powers were equal within measurement error. %
\autoref{fig:PEDOTPSS_mask} diagrams the phase matching mask used in this set of experiments. %
-\begin{dfigure}
+\begin{figure}
\includegraphics[width=0.5\linewidth]{"PEDOT:PSS/mask"}
\caption[PEDOT:PSS 3PE phase matching mask.]{
Phase matching mask used in this experiment.
@@ -107,19 +107,19 @@ that all three excitation pulse powers were equal within measurement error. %
The two stars mark the two output poyntings detected in this work.
}
\label{fig:PEDOTPSS_mask}
-\end{dfigure}
+\end{figure}
\autoref{fig:PEDOTPSS_raw} shows the ten raw 2D delay-delay scans that comprise the primary dataset
described in this section. %
The rows correspond to the two phase matching conditions, as labeled. %
-\begin{dfigure}
+\begin{figure}
\includegraphics[width=\linewidth]{"PEDOT:PSS/raw"}
\caption[PEDOT:PSS 3PE raw data.]{
CAPTION TODO
}
\label{fig:PEDOTPSS_raw}
-\end{dfigure}
+\end{figure}
\subsection{Assignment of zero delay} % ----------------------------------------------------------
@@ -161,37 +161,37 @@ These pulse-overlap effects cause the 3PEPS at small $T$ even without inhomogene
[CITE] %
At long $T$, the average static 3PEPS is 2.5 fs. %
-\begin{dfigure}
+\begin{figure}
\includegraphics[width=\linewidth]{"PEDOT:PSS/delay space"}
\caption[PEDOT:PSS 3PE delay space.]{
CAPTION TODO
}
\label{fig:PEDOTPSS_delay_space}
-\end{dfigure}
+\end{figure}
-\begin{dfigure}
+\begin{figure}
\includegraphics[width=\linewidth]{"PEDOT:PSS/processed"}
\caption[PEDOT:PSS 3PE processed data.]{
CAPTION TODO
}
\label{fig:PEDOTPSS_processed}
-\end{dfigure}
+\end{figure}
-\begin{dfigure}
+\begin{figure}
\includegraphics[width=\linewidth]{"PEDOT:PSS/overtraces"}
\caption[PEDOT:PSS 3PE traces.]{
CAPTION TODO
}
\label{fig:PEDOTPSS_overtraces}
-\end{dfigure}
+\end{figure}
-\begin{dfigure}
+\begin{figure}
\includegraphics[width=\linewidth]{"PEDOT:PSS/traces"}
\caption[PEDOT:PSS 3PE traces.]{
CAPTION TODO
}
\label{fig:PEDOTPSS_traces}
-\end{dfigure}
+\end{figure}
There is a deviation of the TO \RomanNumeral{1}-\RomanNumeral{3} 3PEPS* trace (green line) from the
other traces. %
@@ -238,13 +238,13 @@ Taken together, it is clear that both pure dephasing and ensemble dephasing infl
shift so it is important to find valuse of $T_2^*$ and $\Delta_{\mathsf{inhom}}$ that uniquely
constrain the measured response. %
-\begin{dfigure}
+\begin{figure}
\includegraphics[width=\linewidth]{"PEDOT:PSS/parametric"}
\caption[PEDOT:PSS 3PE traces.]{
CAPTION TODO
}
\label{fig:PEDOTPSS_parametric}
-\end{dfigure}
+\end{figure}
We simulated the $\tau$ trance for a variety of $\Delta_{\mathsf{inhom}}$ and $T_2$ values. %
The results for $\Delta_t = 40$ fs are summarized in \autoref{fig:PEDOTPSS_parametric}. %
@@ -264,7 +264,7 @@ fs. %
Clearly, there is no upper limit that can provide an upper limit for the inhomogeneous
broadening. %
-\begin{dtable}
+\begin{table}
\begin{tabular}{ c | c c c }
$\Delta_t$ (fs) & $T_2$ (fs) & $\hbar T_2^{-1}$ (meV) & $\Delta_{\mathsf{inhom}}$ (meV) \\ \hline
45 & --- & --- & --- \\
@@ -274,15 +274,15 @@ broadening. %
CAPTION TODO
}
\label{tab:PEDOTPSS_table}
-\end{dtable}
+\end{table}
-\begin{dfigure}
+\begin{figure}
\includegraphics[width=\linewidth]{"PEDOT:PSS/agreement"}
\caption[PEDOT:PSS 3PE traces.]{
CAPTION TODO
}
\label{fig:PEDOTPSS_agreement}
-\end{dfigure}
+\end{figure}
Our model system does ans excellent job of reproducing the entire 2D transient within measurement
error (\autoref{fig:PEDOTPSS_agreement}). %