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nam
2016-05-02 13:08:13 +09:00
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35
thesis/chapters/chap3_comet.tex
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@@ -63,20 +63,20 @@ and Cooper~\cite{BernsteinCooper.2013}.
1961 & \sn{4.0}{-6} & Cu & \cite{SardCrowe.etal.1961}\\
1961 & \sn{5.9}{-6} & Cu & \cite{ConversiLella.etal.1961}\\
1962 & \sn{2.2}{-7} & Cu & \cite{ConfortoConversi.etal.1962}\\
1964 & \sn{2.2}{-7} & Cu & \cite{ConversiLella.etal.1961}\\
1972 & \sn{2.6}{-8} & Cu & \cite{ConversiLella.etal.1961}\\
1977 & \sn{4.0}{-10} & S & \cite{ConversiLella.etal.1961}\\
1982 & \sn{7.0}{-11} & S & \cite{ConversiLella.etal.1961}\\
1988 & \sn{4.6}{-12} & Ti & \cite{ConversiLella.etal.1961}\\
1993 & \sn{4.3}{-12} & Ti & \cite{ConversiLella.etal.1961}\\
1995 & \sn{6.5}{-13} & Ti & \cite{ConversiLella.etal.1961}\\
1996 & \sn{4.6}{-11} & Pb & \cite{ConversiLella.etal.1961}\\
2006 & \sn{7.0}{-13} & Au & \cite{ConversiLella.etal.1961}\\
1964 & \sn{2.2}{-7} & Cu & \cite{BartleyDavies.etal.1964}\\
1972 & \sn{2.6}{-8} & Cu & \cite{BrymanBlecher.etal.1972}\\
1977 & \sn{4.0}{-10} & S & \cite{BadertscherBorer.etal.1977}\\
1982 & \sn{7.0}{-11} & S & \cite{BadertscherBorer.etal.1982a}\\
1988 & \sn{4.6}{-12} & Ti & \cite{AhmadAzuelos.etal.1988a}\\
1993 & \sn{4.3}{-12} & Ti & \cite{DohmenGroth.etal.1993}\\
1996 & \sn{4.6}{-11} & Pb & \cite{HoneckerDohmen.etal.1996}\\
2006 & \sn{7.0}{-13} & Au & \cite{Bertl.etal.2006}\\
\bottomrule
%%TODO fix ref
\end{tabular}
\end{center}
\caption{History of \mueconv experiments, reproduced
from~\cite{BernsteinCooper.2013}}
\caption{History of \mueconv experiments with more and more stringent upper
limit.}
\label{tab:mueconv_history}
\end{table}
@@ -94,7 +94,8 @@ muons used in the experiment were \SI{52}{\MeV\per\cc} and
\SI{53}{\MeV\per\cc}, and the momentum spread was 2\%.
\begin{figure}[htbp] \centering
\includegraphics[width=0.85\textwidth]{figs/sindrumII_setup}
\caption{SINDRUM-II set up}
\caption{SINDRUM-II experimental set up, reprinted from
reference~\cite{Bertl.etal.2006} with permission from Springer.}
\label{fig:sindrumII_setup}
\end{figure}
@@ -115,7 +116,9 @@ important in probing better sensitivity.
\begin{figure}[htbp]
\centering
\includegraphics[width=0.55\textwidth]{figs/sindrumII_Au_result}
\caption{SINDRUM-II results}
\caption{SINDRUM-II results showing background events reaching into the
signal region. Reprinted from reference~\cite{Bertl.etal.2006} with
permission from Springer.}
%TODO: explain top and bottom figure
\label{fig:sindrumII_result}
\end{figure}
@@ -353,8 +356,10 @@ Therefore, light material is preferable as muon stopping target.
The conversion rates are normalised to the rate in aluminium. Four models
were considered and noted with letters: D for dipole-interaction-dominated
model, V for vector and S for scalar interactions. The three vertical lines
from left to right correspond to $Z=13$(Al), $Z=22$(Ti), and $Z=82$(Pb)l
respectively.}
from left to right correspond to $Z=13$(Al), $Z=22$(Ti), and $Z=82$(Pb)
respectively. Reprinted figure from
reference~\cite{CiriglianoKitano.etal.2009}. Copyright 2009 by the
American Physical Society.}
\label{fig:comet_mueconv_RateVsZ}
\end{figure}