diff options
Diffstat (limited to 'spectroscopy')
| -rw-r--r-- | spectroscopy/chapter.tex | 12 | 
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
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