From 4ec6538aec763b6cee0f79a0ebcd738aab5a3b41 Mon Sep 17 00:00:00 2001 From: Blaise Thompson Date: Mon, 22 Jan 2018 18:37:19 -0600 Subject: MX2 content grab --- spectroscopy/chapter.tex | 12 +++++++----- 1 file changed, 7 insertions(+), 5 deletions(-) (limited to 'spectroscopy/chapter.tex') 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 -- cgit v1.2.3