\begin{longtable}{p{1.5cm}p{12cm}}
		\hline
		\multicolumn{1}{c}{{\textbf{Section} \texttt{resummation}}} & \multicolumn{1}{c}{{\textbf{Description}}} \\ 
		\hline
\begin{minipage}[t]{0.24\columnwidth}\raggedright
\texttt{makegrid}\strut
\end{minipage} & \begin{minipage}[t]{0.71\columnwidth}\raggedright
If \texttt{.true.}, then MCFM performs
the convolution required to produce beam functions from PDFs and saves
the result as an LHAPDF grid file. The
generated grid files are placed in the directory \texttt{gridoutpath} from
LHAPDF grids in the directory \texttt{gridinpath}. After the grid
generation MCFM stops and should be run subsequently with
\texttt{makegrid = .false.} and \texttt{usegrid = .true.}. When
\texttt{lhapdf\%dopdferrors=.true.} then also grids for the error sets
are generated.\strut
\end{minipage}\tabularnewline
\begin{minipage}[t]{0.24\columnwidth}\raggedright
\texttt{usegrid}\strut
\end{minipage} & \begin{minipage}[t]{0.71\columnwidth}\raggedright
\texttt{.true.} or \texttt{.false.} determines whether pregenerated
LHAPDF interpolation grids should be used for the resummation beam
functions.  Setting \texttt{usegrid = .true.} is much more efficient,
after a suitable run with \texttt{makegrid = .true.} (see above).\strut
\end{minipage}\tabularnewline
\begin{minipage}[t]{0.24\columnwidth}\raggedright
\texttt{gridoutpath}\strut
\end{minipage} & \begin{minipage}[t]{0.71\columnwidth}\raggedright
Output directory for LHAPDF grid files, for example
\texttt{/home/tobias/local/share/LHAPDF/}\strut
\end{minipage}\tabularnewline
\begin{minipage}[t]{0.24\columnwidth}\raggedright
\texttt{gridinpath}\strut
\end{minipage} & \begin{minipage}[t]{0.71\columnwidth}\raggedright
Input directory for LHAPDF grid files, for example
\texttt{/home/tobias/local/share/LHAPDF/}\strut
\end{minipage}\tabularnewline
\begin{minipage}[t]{0.24\columnwidth}\raggedright
\texttt{res\_range}\strut
\end{minipage} & \begin{minipage}[t]{0.71\columnwidth}\raggedright
Integration range of purely resummed part, for example \texttt{0.0 80.0}
for \(q_T\) integration between 0 and 80 GeV.\strut
\end{minipage}\tabularnewline
\begin{minipage}[t]{0.24\columnwidth}\raggedright
\texttt{resexp\_range}\strut
\end{minipage} & \begin{minipage}[t]{0.71\columnwidth}\raggedright
Integration range of fixed-order expanded resummed part, for example
\texttt{1.0 80.0} for \(q_T\) integration between 1 and 80 GeV.\strut
\end{minipage}\tabularnewline
\begin{minipage}[t]{0.24\columnwidth}\raggedright
\texttt{fo\_cutoff}\strut
\end{minipage} & \begin{minipage}[t]{0.71\columnwidth}\raggedright
Lower \(q_T\) cutoff $q_0$ for the fixed-order part. % see Eq.~\eqref{eq:matchingmod} below.
Typically the value should agree with the lower range of \texttt{resexp\_range}.\strut
\end{minipage}\tabularnewline
\begin{minipage}[t]{0.24\columnwidth}\raggedright
\texttt{transitionswitch}\strut
\end{minipage} & \begin{minipage}[t]{0.71\columnwidth}\raggedright
Parameter passed to the plotting routine to modify the transition
function, see text.\strut
\end{minipage}\tabularnewline
\hline
\end{longtable}