first draft r15a xray
This commit is contained in:
@@ -1,2 +1,28 @@
|
||||
\section{Results and discussions}
|
||||
\subsection{Titanium}
|
||||
Number of stopped muons in the natural titanium target was:
|
||||
\begin{equation}
|
||||
N_{\mu} = (88296 \pm 9) \times 10^3 \,.
|
||||
\label{eqn:Nmu_Ti_Tsc}
|
||||
\end{equation}
|
||||
|
||||
Fitting the peak around \SI{931}{keV} in the photon spectrum gives the
|
||||
center of gravity at \SI{931.6 \pm 0.7}{keV} (see~\cref{fig:ti_931keV_fit}),
|
||||
consistent with previously reported value~\cite{Wohlfahrt1981}.
|
||||
Number of $(2p-1s)$ X-rays in the \SI{931.6}{keV} peak is:
|
||||
\begin{equation}
|
||||
N_{931.6} = (20750 \pm 764) \,.
|
||||
\end{equation}
|
||||
|
||||
\begin{figure}[tbp]
|
||||
\centering
|
||||
\includegraphics[width=0.8\textwidth]{figs/ti_931keV_fit}
|
||||
\caption{Fitting $(2p-1s)$ peaks}
|
||||
\label{fig:ti_931keV_fit}
|
||||
\end{figure}
|
||||
|
||||
The emission rate of the $(2p-1s)$ muonic X-rays is calculated as:
|
||||
\begin{equation}
|
||||
R_{Ti} = \frac{N_{931.6}}{A_{931.6} \times N_{\mu} \times f_{capTi}} = 0.90
|
||||
\pm 0.04 \,.
|
||||
\end{equation}
|
||||
|
||||
Reference in New Issue
Block a user