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\begin{longtable}{p{1.5cm}p{12cm}}
\hline
\multicolumn{1}{c}{{\textbf{Section} \texttt{cuts}}} & \multicolumn{1}{c}{{\textbf{Description}}} \\
\hline
\texttt{makecuts} &
If this parameter is set to {\tt .false.}, then
no additional cuts are applied to the events (apart from those in Sections~\ref{basicjets} and \ref{masscuts})
and the remaining parameters in this section are ignored. Otherwise, events will
be rejected according to a set of cuts that is specified below.
Further options may be implemented by editing {\tt src/User/gencuts\_user.f90}. \\
{\tt ptleptmin, etaleptmax} & These specify the values
of $p_{T,{\mathrm{min}}}$ and $|\eta|_{\mathrm{max}}$ for one of the leptons produced
in the process. One can also introduce optional settings \texttt{ptleptmax}
and \texttt{etaleptmin}. \\
{\tt etaleptveto} & This should be specified as a pair of double
precision numbers that indicate a rapidity range that should be excluded
for the lepton that passes the above cuts. \\
{\tt ptminmiss} & Specifies the minimum missing transverse
momentum (coming from neutrinos). \\
{\tt ptlept2min}, \texttt{etalept2max} & These specify
the values of $p_{T,{\mathrm{min}}}$ and $|\eta|_{\mathrm{max}}$ for the remaining
leptons in the process. This allows for staggered cuts where, for
instance, only one lepton is required to be hard and central.
One can also introduce optional settings \texttt{ptlept2max} and
\texttt{etalept2min}. \\
{\tt etalept2veto} & This should be specified as a pair of double
precision numbers (separated by a space) that indicate a rapidity range that should be excluded
for the remaining leptons. \\
\hline
\end{longtable}
%\end{table}
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