diff options
Diffstat (limited to 'spectroscopy')
| -rw-r--r-- | spectroscopy/chapter.tex | 12 |
1 files changed, 5 insertions, 7 deletions
diff --git a/spectroscopy/chapter.tex b/spectroscopy/chapter.tex index 9062e89..3bde7b4 100644 --- a/spectroscopy/chapter.tex +++ b/spectroscopy/chapter.tex @@ -131,7 +131,7 @@ level'' (WMEL) diagram. % Today, double-sided Feynman diagrams are probably most popular, but WMELs will be used in this
document due to author preference. %
-\gls{WMEL} diagrams are drawn using the following rules. %
+WMEL diagrams are drawn using the following rules. %
\begin{denumerate}
\item The energy ladder is represented with horizontal lines - solid for real states and dashed
for virtual states.
@@ -171,12 +171,12 @@ system, each term is roughly ten times smaller than the last. % TODO: cite? \subsection{Homodyne vs heterodyne} % ------------------------------------------------------------
-Two kinds of spectroscopies: 1) \gls{heterodyne} 2) \gls{homodyne}.
-Heterodyne techniques may be \gls{self heterodyne} or explicitly heterodyned with a local
+Two kinds of spectroscopies: 1) heterodyne 2) homodyne.
+Heterodyne techniques may be self heterodyne or explicitly heterodyned with a local
oscillator.
-In all heterodyne spectroscopies, signal goes as $\gls{N}$. %
-In all homodyne spectroscopies, signal goes as $\gls{N}^2$. %
+In all heterodyne spectroscopies, signal goes as $N$. %
+In all homodyne spectroscopies, signal goes as $N^2$. %
This literally means that homodyne signals go as the square of heterodyne signals, which is what we
mean when we say that homodyne signals are intensity level and heterodyne signals are amplitude
level.
@@ -240,8 +240,6 @@ experiment in the Wright Group. % \subsection{Transient absorbance} % --------------------------------------------------------------
-\Gls{transient absorption} (\gls{TA})
-
\subsubsection{Quantitative TA}
Transient absorbance (TA) spectroscopy is a self-heterodyned technique. %
|