\topheading{MCFM references} \label{MCFMrefs} As general references for NLO computations with MCFM, please use: \begin{itemize} \item J.~M.~Campbell and R.~K.~Ellis, \\ %1\cite{Campbell:1999ah} {\it ``An update on vector boson pair production at hadron colliders,''}, \\ Phys.\ Rev.\ D {\bf 60}, 113006 (1999) \href{https://arxiv.org/abs/hep-ph/9905386}{arXiv:hep-ph/9905386}. % \item J.~M.~Campbell, R.~K.~Ellis and C.~Williams, \\ %2\cite{Campbell:2011bn} {\it ``Vector boson pair production at the LHC,''} \\ JHEP {\bf 1107}, 018 (2011) \href{https://arxiv.org/abs/1105.0020}{arXiv:1105.0020 [hep-ph]}. % \item J.~M.~Campbell, R.~K.~Ellis and W.~Giele, \\ %3\cite{Campbell:2015qma} {\it ``A Multi-Threaded Version of MCFM''}, \\ EPJ {\bf C75}, 246 (2015) \href{https://arxiv.org/abs/1503.06182}{arXiv:1503.06182 [hep-ph]}. \end{itemize} When using MCFM 8.0, or later versions, for NNLO calculations of color-singlet processes please refer to: \begin{itemize} \item R.~Boughezal, J.~M.~Campbell, R.~K.~Ellis, \\ C.~Focke, W.~Giele, X.~Liu,~F. Petriello and C.~Williams, \\ %4\cite{Boughezal:2016wmq} {\it ``Color singlet production at NNLO in MCFM''}, \href{https://arxiv.org/abs/1605.08011}{arXiv:1605.08011}. % \item J.~M.~Campbell, R.~K.~Ellis and S.~Seth, \\ %5\cite{Campbell:2022gdq} {it ``Non-local slicing approaches for NNLO QCD in MCFM,''} \href{https://arxiv.org/abs/2202.07738}{arXiv:2202.07738 [hep-ph]} \end{itemize} For calculations of electroweak corrections please refer to: \begin{itemize} \item J.~M.~Campbell, D.~Wackeroth and J.~Zhou, \\ %6\cite{Campbell:2016dks} {\it ``A Study of Weak Corrections to Drell-Yan, Top-quark pair and Di-jet Production at High Energies with MCFM''}, \href{https://arxiv.org/abs/1608.03356}{arXiv:1608.03356}. \end{itemize} When using MCFM 9.0, or later versions please also refer to: \begin{itemize} \item J.~M.~Campbell and Tobias Neumann, \\ %7\cite{Campbell:2019dru} {\it ``Precision Phenomenology with MCFM''}, \href{https://arxiv.org/abs/1909.09117}{arXiv:1909.09117} \end{itemize} Additional references to the program may be used depending on the process under study. The relevant papers are: \begin{itemize} \item J.~M.~Campbell and R.~K.~Ellis, \\ %8\cite{Campbell:2000bg} {\it ``Radiative corrections to Z b anti-b production,''} \\ Phys.\ Rev.\ D {\bf 62}, 114012 (2000) \href{https://arxiv.org/abs/hep-ph/0006304}{arXiv:hep-ph/0006304}. % \item J.~Campbell and R.~K.~Ellis, \\ %9\cite{Campbell:2002tg} {\it ``Next-to-leading order corrections to W + 2jet and Z + 2jet production at hadron colliders,''} \\ Phys.\ Rev.\ D {\bf 65}, 113007 (2002) \href{https://arxiv.org/abs/hep-ph/0202176}{arXiv:hep-ph/0202176}. % \item J.~Campbell, R.~K.~Ellis, F.~Maltoni and S.~Willenbrock, \\ %10\cite{Campbell:2002zm} {\it ``Higgs boson production in association with a single bottom quark,''} \\ Phys.\ Rev.\ D {\bf 67}, 095002 (2003) \href{https://arxiv.org/abs/hep-ph/0204093}{arXiv:hep-ph/0204093}. % \item J.~Campbell, R.~K.~Ellis and D.~L.~Rainwater, \\ %11\cite{Campbell:2003hd} {\it ``Next-to-leading order QCD predictions for W + 2jet and Z + 2jet production at the CERN LHC,''} \\ Phys.\ Rev.\ D {\bf 68}, 094021 (2003) \href{https://arxiv.org/abs/hep-ph/0308195}{arXiv:hep-ph/0308195}. % \item J.~Campbell, R.~K.~Ellis, F.~Maltoni and S.~Willenbrock, \\ %12\cite{Campbell:2003dd} {\it ``Associated production of a Z boson and a single heavy-quark jet,''} \\ Phys.\ Rev.\ D {\bf 69}, 074021 (2004) \href{https://arxiv.org/abs/hep-ph/0312024}{arXiv:hep-ph/0312024}. % \item E.~L.~Berger and J.~Campbell, \\ %13\cite{Berger:2004pca} {\it ``Higgs boson production in weak boson fusion at next-to-leading order,''} \\ Phys.\ Rev.\ D {\bf 70}, 073011 (2004) \href{https://arxiv.org/abs/hep-ph/0403194}{arXiv:hep-ph/0403194}. % \item J.~Campbell, R.~K.~Ellis and F.~Tramontano, \\ %14\cite{Campbell:2004ch} {\it ``Single top production and decay at next-to-leading order,''} \\ Phys.\ Rev.\ D {\bf 70}, 094012 (2004) \href{https://arxiv.org/abs/hep-ph/0408158}{arXiv:hep-ph/0408158}. % \item J.~Campbell and F.~Tramontano, \\ %15\cite{Campbell:2005bb} {\it ``Next-to-leading order corrections to Wt production and decay,''} \\ Nucl.\ Phys.\ B {\bf 726}, 109 (2005) \href{https://arxiv.org/abs/hep-ph/0506289}{arXiv:hep-ph/0506289}. % \item J.~Campbell, R.K.~Ellis, F.~Maltoni and S.~Willenbrock, \\ %16\cite{Campbell:2005zv} {\it ``Production of a $Z$ boson and two jets with one heavy quark tag,''} \\ Phys.\ Rev.\ D {\bf 73}, 054007 (2006) \href{https://arxiv.org/abs/hep-ph/0510362}{arXiv:hep-ph/0510362}. % \item J.~M.~Campbell, R.~Frederix, F.~Maltoni and F.~Tramontano,\\ %17\cite{Campbell:2009ss} {\it ``$t$-channel single top production at hadron colliders,''} \\ Phys. Rev. Lett. {\bf 102} (2009) 182003, \href{https://arxiv.org/abs/0903.0005}{arXiv:0903.0005 [hep-ph]}. % \item J.~M.~Campbell, R.~K.~Ellis and G.~Zanderighi, \\ %18\cite{Campbell:2006xx} {\it ``Next-to-leading order Higgs~$+~2$~jet production via gluon fusion,''} \\ JHEP {\bf 0610}, 028 (2006) \href{https://arxiv.org/abs/hep-ph/0608194}{arXiv:hep-ph/0608194}. % \item J.~Campbell, R.K.~Ellis, F.~Maltoni and S.~Willenbrock, \\ %19\cite{Campbell:2006cu} {\it ``Production of a $W$ boson and two jets with one $b$-quark tag,''} \\ Phys.\ Rev.\ D {\bf 75}, 054015 (2007) \href{https://arxiv.org/abs/hep-ph/0611348}{arXiv:hep-ph/0611348}. % \item J.~M.~Campbell, R.~K.~Ellis, F.~Febres Cordero, F.~Maltoni, L.~Reina, D.~Wackeroth and S.~Willenbrock, \\ %20\cite{Campbell:2008hh} {\it ``Associated Production of a $W$ Boson and One $b$ Jet,''} \\ Phys.\ Rev.\ D {\bf 79}, 034023 (2009) \href{https://arxiv.org/abs/0809.3003}{arXiv:0809.3003 [hep-ph]}. % \item J.~M.~Campbell, R.~K.~Ellis and C.~Williams, \\ %21\cite{Campbell:2010cz} {\it ``Hadronic production of a Higgs boson and two jets at next-to-leading order,''} \\ Phys.\ Rev.\ D {\bf 81} 074023 (2010), \href{https://arxiv.org/abs/1001.4495}{arXiv:1001.4495 [hep-ph]}. % \item S.~Badger, J.~M.~Campbell and R.~K.~Ellis, \\ %22\cite{Badger:2010mg} {\it ``QCD corrections to the hadronic production of a heavy quark pair and a W-boson including decay correlations,''} \\ JHEP {\bf 1103}, 027 (2011) \href{https://arxiv.org/abs/1011.6647}{arXiv:1011.6647 [hep-ph]}]. % \item F.~Caola, J.~M.~Campbell, F.~Febres Cordero, L.~Reina and D.~Wackeroth, \\ %23\cite{Campbell:2011udy} {\it ``NLO QCD predictions for $W+1$ jet and $W+2$ jet production with at least one b jet at the 7 TeV LHC,''} \\ \href{https://arxiv.org/abs/1107.3714}{arXiv:1107.3714 [hep-ph]}. % \item J.~M.~Campbell, R.~K.~Ellis and C.~Williams, \\ %24\cite{Campbell:2011cu} {\it ``Gluon-gluon contributions to W+ W- production and Higgs interference effects,''} \\ JHEP {\bf 1110}, 005 (2011), \href{https://arxiv.org/abs/1107.5569}{arXiv:1107.5569 [hep-ph]}. % \item J.~M.~Campbell and R.~K.~Ellis, \\ %25\cite{Campbell:2012uf} {\it ``Top-quark processes at NLO in production and decay,''} \\ \href{https://arxiv.org/abs/1204.1513}{arXiv:1204.1513 [hep-ph]}, FERMILAB-PUB-12-078-T. % \item J.~M.~Campbell and R.~K.~Ellis, \\ %26\cite{Campbell:2012dh} {\it ``$t \bar{t} W^{\pm}$ production and decay at NLO,''} \\ JHEP {\bf 1207}, 052 (2012), \href{https://arxiv.org/abs/1204.5678}{arXiv:1204.5678 [hep-ph]}. % \item J.~M.~Campbell, H.~B.~Hartanto and C.~Williams,\\ %27\cite{Campbell:2012ft} {\it ``Next-to-leading order predictions for $Z \gamma$+jet and $Z \gamma \gamma$ final states at the LHC''} JHEP {\bf 1211}, 162 (2012), \href{https://arxiv.org/abs/1208.0566}{arXiv:1208.0566 [hep-ph]}. % \item P.~J.~Fox and C.~Williams,\\ %28\cite{Fox:2012ru} {\it ``Next-to-leading order predictions for Dark Matter Production at Hadron Colliders''}, \href{https://arxiv.org/abs/1211.6390}{arXiv:1211.6390 [hep-ph]}. % \item J.~M.~Campbell, R.~K.~Ellis and R.~R{\"o}ntsch, %29\cite{Campbell:2013yla} {\it ``Single top production in association with a Z boson at the LHC,''}, \href{https://arxiv.org/abs/1302.3856}{arXiv:1302.3856 [hep-ph]}. % \item J.~M.~Campbell, R.~K.~Ellis and C.~Williams, %30\cite{Campbell:2016jau} {\it ``Associated Production of a Higgs Boson at NNLO''}, \href{https://arxiv.org/abs/1601.00658}{arXiv:1601.00658 [hep-ph]}. % \item J.~M.~Campbell, R.~K.~Ellis, Ye~Li and C.~Williams, %31\cite{Campbell:2016yrh} {\it ``Predictions for Diphoton Production at the LHC through NNLO in QCD''}, \href{https://arxiv.org/abs/1603.02663}{arXiv:1603.02663 [hep-ph]}. % \item Tobias Neumann and Ciaran Williams,\\ %32\cite{Neumann:2016dny} {\it ``{The Higgs boson at high $p_T$}''}, \href{https://arxiv.org/abs/1609.00367}{arXiv:1609.00367 [hep-ph]}. % \item Tobias Neumann,\\ %33\cite{Neumann:2018bsx} {\it ``NLO Higgs+jet production at large transverse momenta including top quark mass effects''}, \href{https://arxiv.org/abs/1802.02981}{arXiv:1802.02981 [hep-ph]} % \item John M. Campbell, Tobias Neumann and Ciaran Williams,\\ %34\cite{Campbell:2017aul} {\it ``Z gamma Production at NNLO Including Anomalous Couplings''}, \href{https://arxiv.org/abs/1708.02925}{arXiv:1708.02925 [hep-ph]} % \item Tobias Neumann and Zack Edward Sullivan,\\ %35\cite{Neumann:2019kvk} {\it ``Off-Shell Single-Top-Quark Production in the Standard Model Effective Field Theory''}, \href{https://arxiv.org/abs/1903.11023}{arXiv:1903.11023 [hep-ph]} % \item Lucy Budge, John M. Campbell, Giuseppe De Laurentis, R. Keith Ellis, Satyajit Seth,\\ %36\cite{Budge:2020oyl} {\it ``The one-loop amplitudes for Higgs + 4 partons with full mass effects''}, \href{https://arxiv.org/abs/2002.04018}{arXiv:2002.04018 [hep-ph]} \item John M.Campbell, R. Keith Ellis, Satyajit Seth,\\ %\cite{Campbell:2019gmd} {\it ``H + 1 jet production revisited''}, \href{https://arxiv.org/abs/1906.01020}{arXiv:1906.01020} \end{itemize}