From b6aa31ec63513a30fdaaeb2ae18ab13fa1fc60a1 Mon Sep 17 00:00:00 2001
From: Blaise Thompson <blaise@untzag.com>
Date: Fri, 13 Apr 2018 08:46:31 -0500
Subject: 2018-04-13 08:46

---
 PEDOT_PSS/chapter.tex | 42 +++++++++++++++++++++++++++++++-----------
 1 file changed, 31 insertions(+), 11 deletions(-)

(limited to 'PEDOT_PSS')

diff --git a/PEDOT_PSS/chapter.tex b/PEDOT_PSS/chapter.tex
index 10c5af2..b7fba1f 100644
--- a/PEDOT_PSS/chapter.tex
+++ b/PEDOT_PSS/chapter.tex
@@ -1,6 +1,28 @@
-\chapter{PEDOT:PSS}
-
-\section{Introduction}
+\chapter{PEDOT:PSS}  \label{cha:pps}
+
+
+\textit{This Chapter presents content first published in \textcite{HorakErikH2018a}.
+  The authors are:
+  \begin{denumerate}
+    \item Erik H. Horak
+    \item Morgan T. Rea
+    \item Kevin D. Heylman
+    \item David Gelbwaser-Klimovsky
+    \item Semion K. Saikin
+    \item Blaise J. Thompson
+    \item Daniel D. Kohler
+    \item Kassandra A. Knapper
+    \item Wei Wei
+    \item Feng Pan
+    \item Padma Gopalan
+    \item John C. Wright
+    \item Alán Aspuru-Guzik
+    \item Randall H. Goldsmith
+  \end{denumerate}
+  This Chapter focuses on my contribution.  %
+}
+
+\section{Introduction}  % =========================================================================
 
 Poly(3,4-ethylenedioxythiophene)-poly(styrenesulfonate) (PEDOT:PSS) is a transparent, electrically
 conductive (up to 4380 S cm$^{-1}$ \cite{KimNara2013a}) polymer.  %
@@ -15,7 +37,7 @@ even more structural inhomogeneity.  %
 Nonlinear spectroscopy may be able to shed light on the microscopic environment of electronic
 states within PEDOT:PSS.  %
 
-\section{Background}
+\section{Background}  % ===========================================================================
 
 Complex microstructure:
 \begin{enumerate}
@@ -38,7 +60,7 @@ These electronic perturbations arise from injected holes producing a quinoidal d
 over 4-5 monomers of the CP aromatic backbone, collectively called a polaron.  %
 Energetically favorable to be spin-silent bipolaron.  %
 
-\section{Methods}
+\section{Methods}  % ==============================================================================
 
 PEDOT:PSS (Orgacon Dry, Sigma Aldrich) was dropcast onto a glass microscope slide at 1 mg/mL at a
 tilt to ensure homogeneous film formation.  %
@@ -65,7 +87,7 @@ Signal was detected using an InSb photodiode (Teledyne Judson J10D-M204-R01M-3C-
 Four wave mixing was isolated from excitation scatter using dual chopping and digital signal
 processing.  %
 
-\section{Transmittance and reflectance}
+\section{Transmittance and reflectance}  % ========================================================
 
 \autoref{fig:PEDOTPSS_linear} shows the transmission, reflectance, and extinction spectrum of the
 thin film used in this work.  %
@@ -83,7 +105,7 @@ thin film used in this work.  %
 \end{figure}
 \clearpage
 
-\section{Three-pulse echo spectroscopy}  % --------------------------------------------------------
+\section{Three-pulse echo spectroscopy}  % ========================================================
 
 Two dimensional $\tau_{21}, \tau_{22^\prime}$ scans were taken for two phase matching
 configurations: (1) $k_{\mathsf{out}} = k_1 - k_2 + k_{2^\prime}$ (3PE) and (2) $k_{\mathsf{out}} =
@@ -296,8 +318,6 @@ Regardless, these contributions do not affect our analysis.  %
 Extremely fast (single fs) carrier scattering time constants have also been observed for PEDOT-base
 conductive films. [CITES]
 
-\section{Frequency-domain transient grating spectroscopy}  % --------------------------------------
-
-This section describes preliminary, unpublished work accomplished on PEDOT:PSS.  %
-
+\section{Conclusions}  % ==========================================================================
 
+% TODO
\ No newline at end of file
-- 
cgit v1.2.3