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39 lines
2.4 KiB
39 lines
2.4 KiB
\begin{longtable}{p{4.5cm}p{10.5cm}}
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\multicolumn{1}{c}{{\textbf{Section} \texttt{singletop}}} & \multicolumn{1}{c}{{\textbf{Description}}} \\
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\hline
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\texttt{c\_phiq} & Sets real Wilson coefficient of $\Qone$ for processes 164 and 169. See \ref{subsec:offstop}
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and ref.~\cite{Neumann:2019kvk}. \\
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\texttt{c\_phiphi} & Sets real and imaginary part of the $\Qtwo$ Wilson coefficient. \\
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\texttt{c\_tw} & Sets real and imaginary part of the $\Qthree$ Wilson coefficient. \\
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\texttt{c\_bw} & Sets real and imaginary part of the $\Qfour$ Wilson coefficient. \\
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\texttt{c\_tg} & Sets real and imaginary part of the $\Qsix$ Wilson coefficient. \\
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\texttt{c\_bg} & Sets real and imaginary part of the $\Qseven$ Wilson coefficient. \\
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\texttt{lambda} & Scale $\Lambda$, see \ref{subsec:offstop} and ref.~\cite{Neumann:2019kvk}. \\
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\texttt{enable\_lambda4} & Enable contributions of order $1/\Lambda^4$ when set to \texttt{.true.}. \\
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\texttt{disable\_sm} & When set to \texttt{.true.} the pure SM contributions are disabled, and just
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the SM-EFT interference and EFT contributions are calculated. \\
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\texttt{mode\_anomcoup} & When set to \texttt{.true.} at LO one can reproduce results obtained
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without power counting as in the anomalous couplings approach, see \ref{subsec:offstop} and
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ref.~\cite{Neumann:2019kvk}. \\
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\texttt{nnlo\_enable\_light},
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\texttt{nnlo\_enable\_heavy\_prod},
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\texttt{nnlo\_enable\_heavy\_decay},
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\texttt{nnlo\_enable\_interf\_lxh},
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\texttt{nnlo\_enable\_interf\_lxd},
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\texttt{nnlo\_enable\_interf\_hxd},
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\texttt{nnlo\_fully\_inclusive}&
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At NNLO there are several different contributions from vertex
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corrections on the light-quark line, heavy-quark line in production, and
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heavy-quark line in the top-quark decay. Additionally there are one-loop
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times one-loop interference contributions between all three
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contributions. For a fully inclusive calculation without decay
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\texttt{nnlo\_fully\_inclusive} has to
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be set to `.true.` and the decay and decay interference parts have to be
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removed. Additionally jet requirements must be lifted. For further information see
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Section~\ref{single-top-quark-production-and-decay-at-nnlo}. \\
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\hline
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\end{longtable}
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