You can not select more than 25 topics Topics must start with a letter or number, can include dashes ('-') and can be up to 35 characters long.
 
 
 
 
 
 

38 lines
1.6 KiB

\begin{longtable}{p{1.5cm}p{12cm}}
\hline
\multicolumn{1}{c}{{\textbf{Section} \texttt{dipoles}}} & \multicolumn{1}{c}{{\textbf{Description}}} \\
\hline
{\tt aii} &
A double precision variable which can be used to
limit the kinematic range for the subtraction of initial-initial dipoles
as suggested by Trocsanyi and Nagy~\cite{Nagy:2003tz}.
The value {\tt aii=1} corresponds
to standard Catani-Seymour subtraction.\\
{\tt aif} &
A double precision variable which can be used to
limit the kinematic range for the subtraction of initial-final dipoles
as suggested by Trocsanyi and Nagy~\cite{Nagy:2003tz}.
The value {\tt afi=1} corresponds
to standard Catani-Seymour subtraction.\\
{\tt afi} &
A double precision variable which can be used to
limit the kinematic range for the subtraction of final-initial dipoles
as suggested by Trocsanyi and Nagy~\cite{Nagy:2003tz}.
The value {\tt afi=1} corresponds
to standard Catani-Seymour subtraction.\\
{\tt aff} &
A double precision variable which can be used to
limit the kinematic range for the subtraction of final-final dipoles
as suggested by Trocsanyi and Nagy~\cite{Nagy:2003tz}.
The value {\tt aff=1} corresponds
to standard Catani-Seymour subtraction.\\
{\tt bfi} &
A double precision variable which can be used to
limit the kinematic range for the subtraction of final-initial dipoles
in the photon fragmentation case.\\
{\tt bff} &
A double precision variable which can be used to
limit the kinematic range for the subtraction of final-final dipoles
in the photon fragmentation case.\\
\hline
\end{longtable}