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