add progress14
This commit is contained in:
43
progress14/NeutronAnalysis.tex
Normal file
43
progress14/NeutronAnalysis.tex
Normal file
@@ -0,0 +1,43 @@
|
||||
In R2013, two BC501 neutron
|
||||
counters ($5''$ diameter and $5''$ depth) were borrowed from the
|
||||
MuSun experiment, and placed outside the vacuum chamber on
|
||||
both sides of the muon beam and centred on the stopping
|
||||
target. Neutron spectra between 1 to about 20 MeV were obtained. The lower
|
||||
threshold is limited by pulse shape discrimination (PSD) which
|
||||
identifies neutron from photon events. Calibration of the detector
|
||||
energy primarily used Cs-137 and Co-60, however these sources proved
|
||||
inadequate. The Cs-127 Compton edge was too low in energy to be useful
|
||||
and the Co-60 has two overlapping Compton edges. An average of the
|
||||
two edge energies was used for calibration. An AmBe source was
|
||||
originally intended to provide a known neutron spectrum and it did prove
|
||||
useful in providing a 4.19 MeV gamma line for calibration. A ratio of the fast to slow
|
||||
integrated waveform components
|
||||
was used to provide neutron/gamma discrimination.
|
||||
Discrimination is excellent above 1 MeVee, Figure~\ref{psdplot_2013}.
|
||||
Analysis of the R2013 data demonstrated that a waveform digitiser of
|
||||
at least 250 MHz sampling rate is needed to optimise the pulse shape
|
||||
discrimination. A raw neutron spectrum is shown in Figure
|
||||
~\ref{neutron_spectrum}. Initial work on unfolding the
|
||||
spectrum has begun and is described in a later section. \\
|
||||
|
||||
\begin{figure}[btp]
|
||||
\centering
|
||||
\includegraphics[width=0.55\textwidth]{figs/PSD1}
|
||||
\caption{Pulse shape discrimination between
|
||||
neutrons (top band) and gammas (bottom band). The true neutron
|
||||
energy is approximately twice the energy deposited in
|
||||
MeVee.} \label{psdplot_2013}
|
||||
\end{figure}
|
||||
|
||||
|
||||
\begin{figure}[btp]
|
||||
\centering
|
||||
\includegraphics[width=0.55\textwidth]{figs/Neutron_Spectrum}
|
||||
\caption{Raw neutron spectrum from an $Al$
|
||||
target. The horizontal axis is electron equivalent energy
|
||||
which is approximately a factor of 2 greater than the recoil
|
||||
proton energy, which is of course folded by the detector
|
||||
response function. \label{neutron_spectrum}. }
|
||||
\end{figure}
|
||||
|
||||
|
||||
Reference in New Issue
Block a user