From 676aee888e5dc94ba1cc05de869845f4c280c665 Mon Sep 17 00:00:00 2001 From: Blaise Thompson Date: Mon, 27 Nov 2017 22:33:32 -0600 Subject: errata --- instrument/chapter.tex | 14 ++++++++++++-- 1 file changed, 12 insertions(+), 2 deletions(-) (limited to 'instrument/chapter.tex') 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} - - -- cgit v1.2.3