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\begin{longtable}{p{1.5cm}p{12cm}}
\hline
\multicolumn{1}{c}{{\textbf{Section} \texttt{basicjets}}} & \multicolumn{1}{c}{{\textbf{Description}}} \\
\hline
\texttt{inclusive} &
This logical parameter chooses whether the
calculated cross-section should be inclusive in the number of jets
found at NLO. An {\em exclusive}
cross-section contains the same number of jets at next-to-leading
order as at leading order. An {\em inclusive} cross-section may
instead contain an extra jet at NLO. \\
\texttt{algorithm} &
This specifies the jet-finding algorithm that
is used, and can take the values
{\tt ktal} (for the Run II $k_T$-algorithm), {\tt ankt} (for the
``anti-$k_T$'' algorithm~\cite{Cacciari:2008gp}), {\tt cone} (for
a midpoint cone algorithm), {\tt hqrk} (for a simplified cone
algorithm designed for heavy quark processes) and {\tt none} (to
specify no jet clustering at all). The latter option is only a
sensible choice when the leading order cross-section is well-defined
without any jet definition: e.g. the single top process,
$q{\bar q^\prime} \to t{\bar b}$, which is finite as
$p_T({\bar b}) \to 0$. \\
\texttt{ptjetmin}, \texttt{etajetmax} &
These specify the values
of $p_{T,{\mathrm{min}}}$ and $|\eta|_{\mathrm{max}}$ for the
jets that are found by the algorithm. \\
\texttt{etajetmin} &
Optional parameter for setting a minimum jet rapidity $|\eta|_{\mathrm{min}}$. \\
\texttt{ptjetmax} &
Optional parameter for setting maximum jet $p_{T,{\mathrm{max}}}$\\
\texttt{Rcutjet} &
If the final state of the chosen process contains
either quarks or gluons then for each event an attempt will be made
to form them into jets. For this it is necessary to define the
jet separation
\begin{equation} \label{DeltaRdef}
\Delta R=\sqrt{{\Delta \eta}^2 + {\Delta \phi}^2}
\end{equation}
so that after jet combination, all jet pairs are separated by
$\Delta R >$~{\tt Rcutjet}.\\
\texttt{userap} &
Optional parameter for using jet rapidity rather than pseudorapidity when
performing jet cuts. Default is {\tt .true.}. \\
\hline
\end{longtable}