aboutsummaryrefslogtreecommitdiff
path: root/spectroscopy
diff options
context:
space:
mode:
Diffstat (limited to 'spectroscopy')
-rw-r--r--spectroscopy/chapter.tex12
1 files changed, 7 insertions, 5 deletions
diff --git a/spectroscopy/chapter.tex b/spectroscopy/chapter.tex
index 27d763b..9665558 100644
--- a/spectroscopy/chapter.tex
+++ b/spectroscopy/chapter.tex
@@ -1,6 +1,8 @@
% TODO: discuss and cite CerulloGiulio2003.000
% TODO: discuss and cite BrownEmilyJ1999.000
% TODO: cite and discuss Sheik-Bahae 1990 (first z-scan)
+% Modeling of Transient Absorption Spectra in Exciton–Charge-Transfer Systems 10.1021/acs.jpcb.6b09858
+% TODO: Multidimensional Spectral Fingerprints of a New Family of Coherent Analytical Spectroscopies
\chapter{Spectroscopy}
@@ -43,7 +45,7 @@ So-called wave mixing energy level (\gls{WMEL}) diagrams are the most familiar w
spectroscopy for Wright group members. %
\gls{WMEL} diagrams were first proposed by Lee and Albrecht in an appendix to their seminal work
\emph{A Unified View of Raman, Resonance Raman, and Fluorescence Spectroscopy}
-\cite{LeeDuckhwan1985.000}. %
+\cite{LeeDuckhwan1985a}. %
\gls{WMEL} diagrams are drawn using the following rules. %
\begin{enumerate}
\item The energy ladder is represented with horizontal lines - solid for real states and dashed
@@ -66,14 +68,14 @@ spectroscopy for Wright group members. %
\subsection{Reflectivity}
This derivation adapted from \textit{Optical Processes in Semiconductors} by Jacques I. Pankove
-\cite{PankoveJacques1975.000}. %
+\cite{PankoveJacques1975a}. %
For normal incidence, the reflection coefficient is
\begin{equation}
R = \frac{(n-1)^2+k^2}{(n+1)^2+k^2}
\end{equation}
% TODO: finish derivation
-Further derivation adapted from \cite{KumarNardeep2013.000}. %
+Further derivation adapted from \cite{KumarNardeep2013a}. %
To extend reflectivity to a differential measurement
% TODO: finish derivation
@@ -125,10 +127,10 @@ With very short, broad pulses: %
\end{itemize}
This epi-CARS paper might have some useful discussion of non-resonant vs resonant for shorter and
-shorter pulses \cite{ChengJixin2001.000}. %
+shorter pulses \cite{ChengJixin2001a}. %
An excellent discussion of pulse distortion phenomena in broadband time-domain experiments was
-published by \textcite{SpencerAustinP2015.000}. %
+published by \textcite{SpencerAustinP2015a}. %
Another idea in defense of frequency domain is for the case of power studies. %
Since time-domain pulses in-fact possess all colors in them they cannot be trusted as much at