Bibliography

[1]    G. Passarino and M. Veltman, One Loop Corrections for e+ e- Annihilation Into mu+ mu- in the Weinberg Model, Nucl.Phys. B160 (1979) 151.

[2]    G. van Oldenborgh and J. Vermaseren, New Algorithms for One Loop Integrals, Z.Phys. C46 (1990) 425.

[3]    S. Carrazza, R.K. Ellis and G. Zanderighi, QCDLoop: a comprehensive framework for one-loop scalar integrals, Comput. Phys. Commun. 209 (2016) 134 [1605.03181].

[4]    R.K. Ellis and G. Zanderighi, Scalar one-loop integrals for QCD, JHEP 02 (2008) 002 [0712.1851].

[5]    A. van Hameren, OneLOop: For the evaluation of one-loop scalar functions, Comput. Phys. Commun. 182 (2011) 2427 [1007.4716].

[6]    Y. Hida, X.S. Li and D.H. Bailey, “Quad double computation package.” https://crd.lbl.gov/~dhbailey/mpdist/, 2003–2018.

[7]    T. Gehrmann, A. von Manteuffel and L. Tancredi, The two-loop helicity amplitudes for qq¯ V 1V 2 4 leptons, JHEP 09 (2015) 128 [1503.04812].

[8]    L. Naterop, A. Signer and Y. Ulrich, handyG —Rapid numerical evaluation of generalised polylogarithms in Fortran, Comput. Phys. Commun. 253 (2020) 107165 [1909.01656].

[9]    T. Neumann and J. Campbell, Fiducial Drell-Yan production at the LHC improved by transverse-momentum resummation at N4LL+N3LO, 2207.07056.

[10]    J.M. Campbell, R.K. Ellis, T. Neumann and S. Seth, Jet-veto resummation at N3LLp+NNLO in boson production processes, 2301.11768.

[11]    R. Boughezal, J.M. Campbell, R.K. Ellis, C. Focke, W. Giele, X. Liu et al., Color singlet production at NNLO in MCFM, Eur. Phys. J. C 77 (2017) 7 [1605.08011].

[12]    J.M. Campbell, G. De Laurentis, R.K. Ellis and S. Seth, The pp W( ) + γ process at next-to-next-to-leading order, JHEP 07 (2021) 079 [2105.00954].

[13]    S. Badger, J.M. Campbell and R.K. Ellis, QCD corrections to the hadronic production of a heavy quark pair and a W-boson including decay correlations, JHEP 03 (2011) 027 [1011.6647].

[14]    R.K. Ellis and S. Veseli, Strong radiative corrections to W b anti-b production in p anti-p collisions, Phys. Rev. D 60 (1999) 011501 [hep-ph/9810489].

[15]    J.M. Campbell and R.K. Ellis, Next-to-Leading Order Corrections to W+ 2 jet and Z+ 2 Jet Production at Hadron Colliders, Phys. Rev. D 65 (2002) 113007 [hep-ph/0202176].

[16]    J.M. Campbell, R.K. Ellis and D.L. Rainwater, Next-to-leading order QCD predictions for W + 2 jet and Z + 2 jet production at the CERN LHC, Phys. Rev. D 68 (2003) 094021 [hep-ph/0308195].

[17]    Z. Bern, L.J. Dixon and D.A. Kosower, One loop amplitudes for e+ e- to four partons, Nucl. Phys. B513 (1998) 3 [hep-ph/9708239].

[18]    J.M. Campbell and R.K. Ellis, Radiative corrections to Z b anti-b production, Phys. Rev. D 62 (2000) 114012 [hep-ph/0006304].

[19]    J.M. Campbell and R.K. Ellis, An Update on vector boson pair production at hadron colliders, Phys. Rev. D 60 (1999) 113006 [hep-ph/9905386].

[20]    J.M. Campbell, R.K. Ellis and C. Williams, Vector boson pair production at the LHC, JHEP 07 (2011) 018 [1105.0020].

[21]    J.M. Campbell, R.K. Ellis and S. Seth, Non-local slicing approaches for NNLO QCD in MCFM, 2202.07738.

[22]    J.M. Campbell, R.K. Ellis and C. Williams, Associated production of a Higgs boson at NNLO, JHEP 06 (2016) 179 [1601.00658].

[23]    J.M. Campbell, R.K. Ellis and C. Williams, Gluon-Gluon Contributions to W+ W- Production and Higgs Interference Effects, JHEP 10 (2011) 005 [1107.5569].

[24]    J.M. Campbell, R.K. Ellis and C. Williams, Bounding the Higgs Width at the LHC: Complementary Results from H WW, Phys. Rev. D 89 (2014) 053011 [1312.1628].

[25]    J.M. Campbell, R.K. Ellis and C. Williams, Bounding the Higgs Width at the LHC Using Full Analytic Results for gg > ee+μμ+, JHEP 04 (2014) 060 [1311.3589].

[26]    J.M. Campbell, R.K. Ellis, E. Furlan and R. Röntsch, Interference effects for Higgs boson mediated Z-pair plus jet production, Phys. Rev. D 90 (2014) 093008 [1409.1897].

[27]    J.M. Campbell, R.K. Ellis, F. Maltoni and S. Willenbrock, Higgs-Boson Production in Association with a Single Bottom Quark, Phys. Rev. D 67 (2003) 095002 [hep-ph/0204093].

[28]    J.M. Campbell and R.K. Ellis, Top-Quark Processes at NLO in Production and Decay, J. Phys. G42 (2015) 015005 [1204.1513].

[29]    S. Badger, R. Sattler and V. Yundin, One-Loop Helicity Amplitudes for tt¯ Production at Hadron Colliders, Phys. Rev. D83 (2011) 074020 [1101.5947].

[30]    P. Nason, S. Dawson and R.K. Ellis, The Total Cross-Section for the Production of Heavy Quarks in Hadronic Collisions, Nucl. Phys. B303 (1988) 607.

[31]    J.M. Campbell, R.K. Ellis and F. Tramontano, Single top production and decay at next-to-leading order, Phys. Rev. D 70 (2004) 094012 [hep-ph/0408158].

[32]    J.M. Campbell, R. Frederix, F. Maltoni and F. Tramontano, Next-to-Leading-Order Predictions for t-Channel Single-Top Production at Hadron Colliders, Phys. Rev. Lett. 102 (2009) 182003 [0903.0005].

[33]    T. Neumann and Z.E. Sullivan, Off-Shell Single-Top-Quark Production in the Standard Model Effective Field Theory, JHEP 06 (2019) 022 [1903.11023].

[34]    J.M. Campbell and F. Tramontano, Next-to-leading order corrections to Wt production and decay, Nucl. Phys. B 726 (2005) 109 [hep-ph/0506289].

[35]    J.M. Campbell, D. Wackeroth and J. Zhou, Study of weak corrections to Drell-Yan, top-quark pair, and dijet production at high energies with MCFM, Phys. Rev. D94 (2016) 093009 [1608.03356].

[36]    E.L. Berger and J.M. Campbell, Higgs boson production in weak boson fusion at next-to-leading order, Phys. Rev. D 70 (2004) 073011 [hep-ph/0403194].

[37]    J.M. Campbell and R.K. Ellis, Higgs Constraints from Vector Boson Fusion and Scattering, JHEP 04 (2015) 030 [1502.02990].

[38]    J.M. Campbell, R. Frederix, F. Maltoni and F. Tramontano, NLO predictions for t-channel production of single top and fourth generation quarks at hadron colliders, JHEP 10 (2009) 042 [0907.3933].

[39]    T. Melia, K. Melnikov, R. Rontsch and G. Zanderighi, Next-to-leading order QCD predictions for W+W+jj production at the LHC, JHEP 12 (2010) 053 [1007.5313].

[40]    R.K. Ellis and S. Seth, On Higgs boson plus gluon amplitudes at one loop, JHEP 11 (2018) 006 [1808.09292].

[41]    L. Budge, J.M. Campbell, G. De Laurentis, R.K. Ellis and S. Seth, The one-loop amplitudes for Higgs + 4 partons with full mass effects, JHEP 05 (2020) 079 [2002.04018].

[42]    J.M. Campbell, R.K. Ellis and G. Zanderighi, Next-to-Leading order Higgs + 2 jet production via gluon fusion, JHEP 10 (2006) 028 [hep-ph/0608194].

[43]    J.M. Campbell, R.K. Ellis, Y. Li and C. Williams, Predictions for diphoton production at the LHC through NNLO in QCD, JHEP 07 (2016) 148 [1603.02663].

[44]    J.M. Campbell, D.J. Miller and T. Robens, Next-to-Leading Order Predictions for WW+Jet Production, Phys. Rev. D 92 (2015) 014033 [1506.04801].

[45]    J. Campbell, D. Miller and T. Robens, WW + jet at 14 and 100 TeV , PoS ICHEP2016 (2016) 686 [1611.01700].

[46]    J.M. Campbell, G. De Laurentis and R.K. Ellis, Vector boson pair production at one loop: analytic results for the process qq¯¯¯g, JHEP 07 (2022) 096 [2203.17170].

[47]    J.M. Campbell and R.K. Ellis, tt¯W+− production and decay at NLO, JHEP 07 (2012) 052 [1204.5678].

[48]    J. Campbell, R.K. Ellis and R. Röntsch, Single top production in association with a Z boson at the LHC, Phys. Rev. D 87 (2013) 114006 [1302.3856].

[49]    E.W.N. Glover and J.J. van der Bij, Higgs boson pair production via gluon fusion, Nucl. Phys. B309 (1988) 282.

[50]    Particle Data Group collaboration, Review of Particle Physics, Phys. Lett. B667 (2008) 1.

[51]    H. Georgi, Effective field theory and electroweak radiative corrections, Nucl. Phys. B363 (1991) 301.

[52]    F. Maltoni and T. Stelzer, MadEvent: Automatic event generation with MadGraph, JHEP 02 (2003) 027 [hep-ph/0208156].

[53]    M.L. Mangano, M. Moretti, F. Piccinini, R. Pittau and A. Polosa, Alpgen, .

[54]    S. Dittmaier and M. Roth, Lusifer, .

[55]    S. Frixione, Isolated photons in perturbative QCD, Phys. Lett. B429 (1998) 369 [hep-ph/9801442].

[56]    T. Gehrmann, T. Luebbert and L.L. Yang, Calculation of the transverse parton distribution functions at next-to-next-to-leading order, JHEP 06 (2014) 155 [1403.6451].

[57]    G. Billis, M.A. Ebert, J.K.L. Michel and F.J. Tackmann, A toolbox for qT and 0-jettiness subtractions at N3LO, Eur. Phys. J. Plus 136 (2021) 214 [1909.00811].

[58]    T. Becher, M. Neubert and L. Rothen, Factorization and N3LLp+NNLO predictions for the Higgs cross section with a jet veto, JHEP 10 (2013) 125 [1307.0025].

[59]    M. Cacciari, G.P. Salam and G. Soyez, The anti-kt jet clustering algorithm, JHEP 04 (2008) 063 [0802.1189].

[60]    L. Bourhis, M. Fontannaz and J.P. Guillet, Quarks and gluon fragmentation functions into photons, Eur. Phys. J. C2 (1998) 529 [hep-ph/9704447].

[61]    A. Gehrmann-De Ridder and E.W.N. Glover, Final state photon production at LEP, Eur. Phys. J. C7 (1999) 29 [hep-ph/9806316].

[62]    J. Campbell and T. Neumann, Precision Phenomenology with MCFM, JHEP 12 (2019) 034 [1909.09117].

[63]    Z. Nagy, Next-to-leading order calculation of three jet observables in hadron hadron collision, Phys. Rev. D68 (2003) 094002 [hep-ph/0307268].

[64]    G.P. Salam, Towards Jetography, Eur. Phys. J. C 67 (2010) 637 [0906.1833].

[65]    Y.L. Dokshitzer, G.D. Leder, S. Moretti and B.R. Webber, Better jet clustering algorithms, JHEP 08 (1997) 001 [hep-ph/9707323].

[66]    M. Wobisch and T. Wengler, Hadronization corrections to jet cross-sections in deep inelastic scattering, in Workshop on Monte Carlo Generators for HERA Physics (Plenary Starting Meeting), pp. 270–279, 4, 1998 [hep-ph/9907280].

[67]    S. Catani, Y.L. Dokshitzer, M.H. Seymour and B.R. Webber, Longitudinally invariant Kt clustering algorithms for hadron hadron collisions, Nucl. Phys. B 406 (1993) 187.

[68]    S.D. Ellis and D.E. Soper, Successive combination jet algorithm for hadron collisions, Phys. Rev. D 48 (1993) 3160 [hep-ph/9305266].

[69]    J.M. Campbell, S. Höche and C.T. Preuss, Accelerating LHC phenomenology with analytic one-loop amplitudes: A C++ interface to MCFM, Eur. Phys. J. C 81 (2021) 1117 [2107.04472].

[70]    L.J. Dixon, Z. Kunszt and A. Signer, Helicity amplitudes for O(αs) production of W+W, W±Z, ZZ, W±γ, or pairs at hadron colliders, Nucl. Phys. B531 (1998) 3 [hep-ph/9803250].

[71]    L.J. Dixon, Z. Kunszt and A. Signer, Vector boson pair production in hadronic collisions at order αs : Lepton correlations and anomalous couplings, Phys. Rev. D60 (1999) 114037 [hep-ph/9907305].

[72]    R.K. Ellis, W.J. Stirling and B.R. Webber, QCD and collider physics, Camb. Monogr. Part. Phys. Nucl. Phys. Cosmol. 8 (1996) 1.

[73]    A. Djouadi, V. Driesen, W. Hollik and A. Kraft, The Higgs photon - Z boson coupling revisited, Eur. Phys. J. C1 (1998) 163 [hep-ph/9701342].

[74]    S. Goria, G. Passarino and D. Rosco, The Higgs Boson Lineshape, Nucl. Phys. B864 (2012) 530 [1112.5517].

[75]    G. Passarino, C. Sturm and S. Uccirati, Higgs Pseudo-Observables, Second Riemann Sheet and All That, Nucl. Phys. B834 (2010) 77 [1001.3360].

[76]    J.G. Korner and Z. Merebashvili, One loop corrections to four point functions with two external massive fermions and two external massless partons, Phys. Rev. D66 (2002) 054023 [hep-ph/0207054].

[77]    J. Campbell, T. Neumann and Z. Sullivan, Single-top-quark production in the t-channel at NNLO, JHEP 02 (2021) 040 [2012.01574].

[78]    J. Campbell, T. Neumann and Z. Sullivan, Testing parton distribution functions with t-channel single-top-quark production, Phys. Rev. D 104 (2021) 094042 [2109.10448].

[79]    I.R. Blokland, A. Czarnecki, M. Slusarczyk and F. Tkachov, Next-to-next-to-leading order calculations for heavy-to-light decays, Phys. Rev. D 71 (2005) 054004 [hep-ph/0503039].

[80]    A. Czarnecki, QCD corrections to the decay t — > W b in dimensional regularization, Phys. Lett. B 252 (1990) 467.

[81]    T. Neumann and C. Williams, The Higgs boson at high pT, Phys. Rev. D95 (2017) 014004 [1609.00367].

[82]    T. Neumann, NLO Higgs+jet production at large transverse momenta including top quark mass effects, J. Phys. Comm. 2 (2018) 095017 [1802.02981].

[83]    R.K. Ellis, I. Hinchliffe, M. Soldate and J.J. van der Bij, Higgs Decay to tau+ tau-: A Possible Signature of Intermediate Mass Higgs Bosons at the SSC, Nucl. Phys. B 297 (1988) 221.

[84]    U. Baur and E.W.N. Glover, Higgs Boson Production at Large Transverse Momentum in Hadronic Collisions, Nucl. Phys. B 339 (1990) 38.

[85]    S.P. Jones, M. Kerner and G. Luisoni, Next-to-Leading-Order QCD Corrections to Higgs Boson Plus Jet Production with Full Top-Quark Mass Dependence, Phys. Rev. Lett. 120 (2018) 162001 [1802.00349].

[86]    X. Chen, A. Huss, S.P. Jones, M. Kerner, J.N. Lang, J.M. Lindert et al., Top-quark mass effects in H+jet and H+2 jets production, JHEP 03 (2022) 096 [2110.06953].

[87]    R. Bonciani, V. Del Duca, H. Frellesvig, M. Hidding, V. Hirschi, F. Moriello et al., Next-to-leading-order QCD Corrections to Higgs Production in association with a Jet, 2206.10490.

[88]    V. Ravindran, J. Smith and W.L. Van Neerven, Next-to-leading order QCD corrections to differential distributions of Higgs boson production in hadron hadron collisions, Nucl. Phys. B634 (2002) 247 [hep-ph/0201114].

[89]    C.R. Schmidt, H ggg(gqq) at two loops in the large-Mt limit, Phys. Lett. B413 (1997) 391 [hep-ph/9707448].

[90]    D. de Florian, M. Grazzini and Z. Kunszt, Higgs production with large transverse momentum in hadronic collisions at next-to-leading order, Phys. Rev. Lett. 82 (1999) 5209 [hep-ph/9902483].

[91]    C.J. Glosser and C.R. Schmidt, Next-to-leading corrections to the Higgs boson transverse momentum spectrum in gluon fusion, JHEP 12 (2002) 016 [hep-ph/0209248].

[92]    J.M. Campbell, R.K. Ellis and S. Seth, H + 1 jet production revisited, JHEP 10 (2019) 136 [1906.01020].

[93]    R. Kleiss and W.J. Stirling, Top quark production at hadron colliders: Some useful formulae, Z. Phys. C40 (1988) 419.

[94]    J.M. Campbell, R.K. Ellis, F. Maltoni and S. Willenbrock, Associated production of a Z Boson and a single heavy quark jet, Phys. Rev. D 69 (2004) 074021 [hep-ph/0312024].

[95]    J.M. Campbell, R.K. Ellis and C. Williams, Direct Photon Production at Next-to–Next-to-Leading Order, Phys. Rev. Lett. 118 (2017) 222001 [1612.04333].

[96]    J.M. Campbell, R.K. Ellis and C. Williams, Driving missing data at the LHC: NNLO predictions for the ratio of γ + j and Z + j, Phys. Rev. D 96 (2017) 014037 [1703.10109].

[97]    J.M. Campbell, J. Rojo, E. Slade and C. Williams, Direct photon production and PDF fits reloaded, Eur. Phys. J. C 78 (2018) 470 [1802.03021].

[98]    Z. Bern, L.J. Dixon and C. Schmidt, Isolating a light Higgs boson from the diphoton background at the CERN LHC, Phys. Rev. D66 (2002) 074018 [hep-ph/0206194].

[99]    T. Neumann, The diphoton qT spectrum at N3LL + NNLO, Eur. Phys. J. C 81 (2021) 905 [2107.12478].

[100]    T. Becher and T. Neumann, Fiducial qT resummation of color-singlet processes at N3LL+NNLO, JHEP 03 (2021) 199 [2009.11437].

[101]    F. Caola, A. Von Manteuffel and L. Tancredi, Diphoton Amplitudes in Three-Loop Quantum Chromodynamics, Phys. Rev. Lett. 126 (2021) 112004 [2011.13946].

[102]    M.-x. Luo, T.-Z. Yang, H.X. Zhu and Y.J. Zhu, Unpolarized quark and gluon TMD PDFs and FFs at N3LO, JHEP 06 (2021) 115 [2012.03256].

[103]    M.A. Ebert, B. Mistlberger and G. Vita, Transverse momentum dependent PDFs at N3LO, JHEP 09 (2020) 146 [2006.05329].

[104]    M.-x. Luo, T.-Z. Yang, H.X. Zhu and Y.J. Zhu, Quark Transverse Parton Distribution at the Next-to-Next-to-Next-to-Leading Order, Phys. Rev. Lett. 124 (2020) 092001 [1912.05778].

[105]    J.M. Campbell and C. Williams, Triphoton production at hadron colliders, Phys. Rev. D 89 (2014) 113001 [1403.2641].

[106]    T. Gehrmann and L. Tancredi, Two-loop QCD helicity amplitudes for qq¯ W±γ and qq¯ Z0γ, JHEP 02 (2012) 004 [1112.1531].

[107]    D. De Florian and A. Signer, W gamma and Z gamma production at hadron colliders, Eur. Phys. J. C16 (2000) 105 [hep-ph/0002138].

[108]    J.M. Campbell, T. Neumann and C. Williams, Production at NNLO Including Anomalous Couplings, JHEP 11 (2017) 150 [1708.02925].

[109]    J.M. Campbell, R.K. Ellis, F. Maltoni and S. Willenbrock, Production of a Z boson and two jets with one heavy-quark tag, Phys. Rev. D 73 (2006) 054007 [hep-ph/0510362].

[110]    J.M. Campbell, R.K. Ellis, F. Febres Cordero, F. Maltoni, L. Reina, D. Wackeroth et al., Associated Production of a W Boson and One b Jet, Phys. Rev. D79 (2009) 034023 [0809.3003].

[111]    J.M. Campbell, F. Caola, F. Febres Cordero, L. Reina and D. Wackeroth, NLO QCD predictions for W + 1 jet and W + 2 jet production with at least one b jet at the 7 TeV LHC, Phys. Rev. D86 (2012) 034021 [1107.3714].

[112]    J. Teunissen, config_fortran - A configuration file parser for Fortran, 2019.

[113]    D. van Vugt and K. Beljaars, Modern fortran implementation of a Sobol sequence, 2016.

[114]    S. Joe and F.Y. Kuo, Sobol sequence direction numbers, 2010.