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.
 
 
 
 
 
 

52 lines
3.3 KiB

\begin{longtable}{p{1.5cm}p{12cm}}
\hline
\multicolumn{1}{c}{{\textbf{Section} \texttt{nnlo}}} & \multicolumn{1}{c}{{\textbf{Description}}} \\
\hline
\texttt{taucut} &
Optional. This sets the value of the jettiness variable
$\tau_{\text{cut}}$, as a multiple of the invariant mass of the Born system,
i.e.
\begin{equation}
\tau_{\text{cut}} = \texttt{taucut} \times Q
\end{equation}
This variable separates the resolved and unresolved regions in NNLO
calculations that use zero-jettiness. The default value results
in total inclusive cross sections with less than $1\%$ residual cutoff effects. \\
\texttt{tcutarray} &
Optional. Array that specifies multiple taucut values that should be sampled
on the fly in addition to the nominal taucut value. Both larger and smaller
values than the nominal one can be specified, although uncertainties for
smaller values will be large. We generally do not recommend smaller values
than the nominal one chosen with \texttt{taucut}. Default values are chosen
to be $2,4,8,20,40$ times the nominal choice of \texttt{taucut}. \\
\texttt{dynamictau} &
Optional. If \texttt{.false.}, the \texttt{taucut} value specified
is not multiplied by the invariant mass of the Born system. Default is \texttt{.true.}. \\
\texttt{useqt} & Flag to use $q_T$ slicing, rather than
0-jettiness, in the calculation of NNLO contributions.
Default is \texttt{.false.} \\
\texttt{useGLY} & If \texttt{.true.}, implement non-local $q_T$ subtraction using formulas from Gehrmann et al.(GLY)~\cite{Gehrmann:2014yya}.
Default is \texttt{.true.} when \texttt{useqt} is enabled. If \texttt{.false},
implement non-local $q_T$ subtraction using formulas from Billis et al.(BEMT)~\cite{Billis:2019vxg}. \\
\texttt{qtcut} & If \texttt{useqt} is enabled, the value of the slicing parameter, defined
in the same way as \texttt{taucut} described above. \\
\texttt{tauboost} & When using 0-jettiness, perform the slicing cut in the
centre-of-mass of the color singlet system. Default is \texttt{.true.} \\
\texttt{incpowcorr} & When using 0-jettiness, include leading power corrections
in the below-cut calculation. Default is \texttt{.false.} \\
\texttt{onlypowcorr} & When using 0-jettiness, only compute the power corrections
to the below-cut calculation. Default is \texttt{.false.} \\
\texttt{usept} & This flag has two separate uses. In a fixed-order sliciing calculation,
e.g. {\tt part} is equal to {\tt snlo} or {\tt nnlo}, the code uses $p_T^{veto}$ slicing, rather than
0-jettiness, in the calculation of higher-order contributions.
In a resummed calculation, e.g. {\tt part} is equal to {\tt resNLO} or {\tt resNNLO},
it enables the use of $p_T^{veto}$ resummation rather that $q_T$ resummation.
In this case the value of the jet veto (\texttt{ptveto}) is set separately in the
\texttt{resummation} block.
Default is \texttt{.false.} \\
\texttt{useBNR} & Implements $p_T^{veto}$ formalism using the refactorized approach of
Ref.~\cite{Becher:2013xia}. Otherwise uses original `$B \times B \times S$' factorization
of below-cut cross-section into beam and soft functions (that gives identical results).
Default is \texttt{.true.} \\
\hline
\end{longtable}