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| author | Blaise Thompson <blaise@untzag.com> | 2018-04-04 11:06:13 -0500 |
|---|---|---|
| committer | Blaise Thompson <blaise@untzag.com> | 2018-04-04 11:06:13 -0500 |
| commit | dc15adadcb2b7560d982c3aee0ef319b50d9d362 (patch) | |
| tree | 28432069e55a967f8c7be19f4b5393d8560c7dae /active_correction/chapter.tex | |
| parent | 272de2372369fe74fa7f4d281e76a52454a7d34a (diff) | |
remove gls
Diffstat (limited to 'active_correction/chapter.tex')
| -rw-r--r-- | active_correction/chapter.tex | 2 |
1 files changed, 1 insertions, 1 deletions
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:
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