new unit for speed of light
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@@ -244,8 +244,8 @@ In this analysis, a subset of runs from \numrange{2808}{2873} with the
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\item a thicker target gives better statistics because of a higher
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muon rate available at a higher momentum and less scattering.
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\end{itemize}
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Muons with momentum of \SI{30.52}{\MeV\per\cc}, 3\%-FWHM spread (scaling factor of
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1.09, normalised to \SI{28}{\MeV\per\cc}) were used for this target after
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Muons with momentum of \SI{30.52}{\MeV\per\hepclight}, 3\%-FWHM spread (scaling factor of
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1.09, normalised to \SI{28}{\MeV\per\hepclight}) were used for this target after
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a momentum scanning as described in the next subsection.
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\subsection{Momentum scan for the 100-\si{\um} aluminium target}
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@@ -260,7 +260,7 @@ in \cref{tab:al100_scan}.
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\begin{center}
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\begin{tabular}{cccc}
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\toprule
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\textbf{Momentum (\si{\MeV\per\cc})} & \textbf{Scaling factor} & \textbf{Runs}
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\textbf{Momentum (\si{\MeV\per\hepclight})} & \textbf{Scaling factor} & \textbf{Runs}
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& \textbf{Length (s)}\\
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\midrule
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29.12 & 1.04 & \numrange{2609}{2613} &2299\\
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