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

---
 PEDOT_PSS/chapter.tex | 14 ++++++++------
 1 file changed, 8 insertions(+), 6 deletions(-)

(limited to 'PEDOT_PSS/chapter.tex')

diff --git a/PEDOT_PSS/chapter.tex b/PEDOT_PSS/chapter.tex
index 24702d1..622f8e4 100644
--- a/PEDOT_PSS/chapter.tex
+++ b/PEDOT_PSS/chapter.tex
@@ -37,14 +37,16 @@ even more structural inhomogeneity.
 In summary, PEDOT:PSS has a complex, nested microstructure.  %
 From smallest to largest:
 \begin{ditemize}
-  \item PEDOT oligomers (6---18-mers) % [CITE 14]
+  \item PEDOT oligomers (6---18-mers) \cite{KirchmeyerStephan2005a}
   \item these oligomers $\pi$-stack to form small nanocrystalites, 3 to 14 oligomers for pristine
-    films to as many as 13---14 oligomers for more conductive solvent treated films % [CITE 15]
+    films to as many as 13---14 oligomers for more conductive solvent treated films
+    \cite{TakanoTakumi2012a}
   \item nanocrystallites then arrange into globular conductive particles in a pancake-like shape
-   %   [CITE 16, 17]
+    \cite{NardesAlexandreMantovani2007a, NardesAlexandreMantovani2008a}
   \item these particles themselves are then linked via PSS-rich domains and assembled into
-    nanofibril geometry akin to a string of pearls  %[CITE 6, 21]
-  \item nanofibrils interweave to form thin films, with PSS capping layer at surface %[CITE 19, 22]
+    nanofibril geometry akin to a string of pearls \cite{KimNara2013a, vandeRuitKevin2013a}
+  \item nanofibrils interweave to form thin films, with PSS capping layer at surface
+    \cite{TimpanaroS2004a}
 \end{ditemize}
 
 In order to be conductive, PEDOT:PSS needs to have good spatial and energetic overlap between
@@ -283,7 +285,7 @@ The lines of constant $T_2$ span from $\Delta_{\mathsf{inhom}} = 0$ (green left
 the limit $\Delta_{\mathsf{inhom}} \rightarrow \infty$ (blue right ends of curves).  %
 The lines of constant $T_2$ demonstrate that ensemble dephasing reduces the transient duration and
 introduces a peak shift.  %
-The influence of inhomogeneity on the observables vanishes as $T_2 \rightarrow \infty$. % 
+The influence of inhomogeneity on the observables vanishes as $T_2 \rightarrow \infty$. %
 
 We preformed simulations analogus to those in \autoref{pps:fig:parametric} for pulse durations
 longer and smaller than $\Delta_t = 40$ fs.  %
-- 
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