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70 lines
3.2 KiB
70 lines
3.2 KiB
\midheading{References}
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The program has been
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developed over a number of years and results have been presented in
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a number of published papers. The papers describing the original
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code and the most significant developments in the NLO implementation are:
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\begin{itemize}
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\item J.~M.~Campbell and R.~K.~Ellis, \\
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{\it ``An update on vector boson pair production at hadron colliders,''} \\
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Phys.\ Rev.\ D {\bf 60}, 113006 (1999)
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\href{https://arxiv.org/abs/hep-ph/9905386}{arXiv:hep-ph/9905386}.
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\item J.~M.~Campbell, R.~K.~Ellis and C.~Williams, \\
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{\it ``Vector boson pair production at the LHC,''} \\
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JHEP {\bf 1107}, 018 (2011)
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\href{https://arxiv.org/abs/1105.0020}{arXiv:1105.0020 [hep-ph]}.
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\item J.~M.~Campbell, R.~K.~Ellis and W.~Giele, \\
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{\it ``A Multi-Threaded Version of MCFM''}, \\
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EPJ {\bf C75}, 246 (2015)
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\href{https://arxiv.org/abs/1503.06182}{arXiv:1503.06182 [hep-ph]}.
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\end{itemize}
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As of \textbf{v8.0} MCFM can also compute selected color-singlet processes through NNLO in
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QCD perturbation theory. The processes available at this precision, as well as
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benchmark numbers, are detailed in Section~\ref{sec:scetqt}. When using MCFM 8.0 or newer
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for NNLO calculations please refer to:
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\begin{itemize}
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\item
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R.~Boughezal, J.~M.~Campbell, R.~K.~Ellis, \\
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C.~Focke, W.~Giele, X.~Liu,~F. Petriello and C.~Williams, \\
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{\it ``Color singlet production at NNLO in MCFM''},
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\href{https://arxiv.org/abs/1605.08011}{arXiv:1605.08011}.
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\end{itemize}
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A significant overhaul of MCFM was undertaken in \textbf{v9.0} of MCFM. If you use
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this version or newer please cite
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\begin{itemize}
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\item John M. Campbell and Tobias Neumann,\\
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{\it ``Precision Phenomenology with MCFM''},
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\href{https://arxiv.org/abs/1909.09117}{arXiv:1909.09117}
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\end{itemize}
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Version \textbf{10.0} includes SCET-based $q_T$ resummation and is called CuTe-MCFM when this
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feature is used. When you use the $q_T$ resummation please cite
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\begin{itemize}
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\item Thomas Becher and Tobias Neumann,\\
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{\it ``Fiducial $q_T^2$ resummation of color-singlet processes at N$^3$LL+NNLO''},
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\href{https://arxiv.org/abs/2009.11437}{arXiv:2009.11437}
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\end{itemize}
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The manual for the resummation functionality can be found in \texttt{cute-mcfm.pdf}.
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Version \textbf{10.1} includes a C++ interface to many of the 1-loop matrix elements
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included in the code. When you use this functionality please cite
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\begin{itemize}
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\item
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John M. Campbell, Stefan H{\"o}che and Christian T. Preuss,\\
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{\it Accelerating LHC phenomenology with analytic one-loop amplitudes: A C++ interface to MCFM},
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\href{https://arxiv.org/abs/2107.04472}{arXiv:2107.04472}
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\end{itemize}
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A guide to the structure of the interface is included in this paper.
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Version \textbf{10.2} includes a more complete treatment of color singlet production
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processes at NNLO, expecially colour singlet processes involving pairs of bosons.
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\begin{itemize}
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\item
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John M. Campbell, R. Keith Ellis and Satyajit Seth,\\
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{\it ``Non-local slicing approaches for NNLO QCD in MCFM''},
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\href{https://arxiv.org/abs/2202.07738}{arXiv:2202.07738 [hep-ph]}
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\end{itemize}
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%Other relevant references, corresponding to publications associated with the
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%implementation of specific processes at NLO and NNLO, are listed
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%in \ref{MCFMrefs}.
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