remove gls

4 files changed, 10 insertions, 12 deletions

diff --git a/acquisition/chapter.tex b/acquisition/chapter.tex
index fe3c4da..0d3d1c5 100644
--- a/acquisition/chapter.tex
+++ b/acquisition/chapter.tex
@@ -65,7 +65,7 @@ It is open source, developed on GitHub.  % TODO: cite PyCMDS on github
 PyCMDS is used to drive both of the MR-CMDS instruments maintained by the Wright Group: the ``fs

 table'', focused on semiconductor photophysics, and the ``ps table'', focused on molecular

 systems.  %

-In the Wright Group, \gls{PyCMDS} replaces the old acquisition softwares `ps control', ritten by

+In the Wright Group, PyCMDS replaces the old acquisition softwares `ps control', ritten by

 Kent Meyer and `Control for Lots of Research in Spectroscopy' written by Schuyler Kain.

 

 When PyCMDS starts up, the GUI is constructed out of modules depending on which hardware and

@@ -659,10 +659,10 @@ central conceit of PyCMDS.  %
 \subsection{Ideal Axis Positions} \label{acq:sec:ideal_axis_positions}  % -------------------------

 

 Frequency domain multidimensional spectroscopy is a time-intensive process.  %

-A typical \gls{pixel} takes between one-half second and three seconds to acquire.  %

+A typical pixel takes between one-half second and three seconds to acquire.  %

 Depending on the exact hardware being scanned and signal being detected, this time may be mostly

 due to hardware motion or signal collection.  %

-Due to the \gls{curse of dimensionality}, a typical three-dimensional CMDS experiment contains

+Due to the curse of dimensionality, a typical three-dimensional CMDS experiment contains

 roughly 100,000 pixels.  %

 CMDS hardware is transiently-reliable, so speeding up experiments is a crucial component of

 unlocking ever larger dimensionalities and higher resolutions.  %

diff --git a/active_correction/chapter.tex b/active_correction/chapter.tex
index 40e0e56..76ae49d 100644
--- a/active_correction/chapter.tex
+++ b/active_correction/chapter.tex
@@ -101,7 +101,7 @@ The phase of signal is then
 The phase of each excitation field can also be written:

 \begin{eqnarray}

 \Phi_{1} &=& \mathrm{e}^0 \\

-\Phi_{2} &=& \mathrm{e}^{-\tau_2\gls{omega}} \\

+\Phi_{2} &=& \mathrm{e}^{-\tau_2\omega} \\

 \Phi_{2^\prime} &=& \mathrm{e}^{-\tau_{2^\prime}\omega}

 \end{eqnarray}

 The cross term between scatter and signal is the product of $\Phi_\mathrm{sig}$ and $\Phi_\mathrm{scatter}$. The cross terms are:

diff --git a/software/chapter.tex b/software/chapter.tex
index 5888073..0027c5f 100644
--- a/software/chapter.tex
+++ b/software/chapter.tex
@@ -281,7 +281,7 @@ class Person():
         if food == self.favorite_food:

             return 'yum! my favorite'

         elif food == self.hated_food:

-            return 'gross---no thank you'''''''''

+            return 'gross---no thank you'

         else:

             return 'meh''

 \end{codefragment}

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.  %