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| author | Blaise Thompson <blaise@untzag.com> | 2017-11-27 22:33:32 -0600 |
|---|---|---|
| committer | Blaise Thompson <blaise@untzag.com> | 2017-11-27 22:33:32 -0600 |
| commit | 676aee888e5dc94ba1cc05de869845f4c280c665 (patch) | |
| tree | 5d5e520b061be0e3cdfb1b8eb185b94402ea6297 /instrument | |
| parent | b4d2785e395ee915043b1c7b74d4a16c65f9cef8 (diff) | |
errata
Diffstat (limited to 'instrument')
| -rw-r--r-- | instrument/chapter.tex | 14 |
1 files changed, 12 insertions, 2 deletions
diff --git a/instrument/chapter.tex b/instrument/chapter.tex index ffb8eb5..179a629 100644 --- a/instrument/chapter.tex +++ b/instrument/chapter.tex @@ -196,6 +196,18 @@ This is a well known strategy for removing unwanted interference terms \cite{Spe \subsection{Normalization of dual-chopped self-heterodyned signal}
+%\begin{table}[!htb]
+% \centering
+% \renewcommand{\arraystretch}{1.5}
+%\begin{array}{r | c | c | c | c }
+% & A & B & C & D \\ \hline
+% \text{signal} & S_A=V_A^S & S_B=R^SC^1I_B^S & S_C=R^S(C^1) & S_D=R^SC^2I_D^S \\ \hline
+% \text{source 1} & M_A^1=V_A^1 & M_B=R^1I_B^1 & M_C^1=R^1I_C^1 & M_D^1=V_D^1 \\ \hline
+% \text{source 2} & M_A^2=V_A^2 & M_B^2=V_B^2 & M_C^2=R^2I_C^2 & M_D^2=R^2I_D^2
+%\end{array}
+% \caption{CAPTION}
+%\end{table}
+
Shot-by-shot normalization is not trivial for these experiments. %
As in table above, with 1 as pump and 2 as probe. %
@@ -236,5 +248,3 @@ Now, substituting in BRAZARD formalism: \section{Optomechanics} % ------------------------------------------------------------------------
\subsection{Automated Neutral Density Wheels}
-
-
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